2000 (with abstract) |
|
▼ Ordered by first author |
1. K.
Ajito, M. Morita, and K. Torimitsu
"Investigation
of the molecular extraction process in single subpicoliter droplets using a
near-infrared laser Raman trapping system"
Anal.
Chem. 72 (19), 4721-4725 (2000).
ABSTRACT: The
near-infrared (NIR) laser Raman trapping system was applied to study
liquid-liquid extraction in a single droplet in a subpicoliter range. The
system trapped a single subpicoliter toluene droplet in water using the NIR
laser beam and provided time-dependent optical images of the droplet during
liquid-liquid extraction. The size of the trapped droplet gradually increased
after p-nonylphenol solution was added in water. The Raman spectra of the
droplet prove that the increase of the droplet size was caused by the
absorption of p-nonylphenol from the water. The distribution coefficient of
p-nonylphenol in the subpicoliter droplet was much higher than that in bulk
solution.
2. K.
Ajito and K. Torimitsu
"Spectroscopy
of organic and biological single particles on nanometer and micrometer scales
using a near-infrared laser Raman trapping system"
in
Microbeam Analysis 2000, Proceedings, Institute Of Physics Conference
Series Vol. 165 (Iop Publishing Ltd, Bristol, 2000), pp. 21-22.
ABSTRACT:
3. L.
Alff, S. Kleefisch, S. Meyer, U. Schoop, A. Marx, H. Sato, M. Naito, and R.
Gross
"Determination
of the order parameter symmetry in hole and electron doped cuprate
superconductors"
Physica
B 284, 591-592 (2000).
ABSTRACT: It
is well established that the order parameter symmetry in the hole-doped
high-temperature superconductors (HTS) is of d-wave type. For the
electron-doped HTS one could expect to find the same order parameter symmetry
because both systems have the copper oxygen planes in common. However, our experiments
based on bicrystal grain boundary junctions (GBJs) show the absence of zero
energy Andreev bound states as well as a s-wave like temperature dependence of
the London penetration depth thereby excluding a d-wave symmetry of the order
parameter in the electron-doped cuprates. At present, it is not fully
established whether the electron-doped HTS have an isotropic or an anisotropic
s-wave symmetry of the order parameter. (C) 2000 Elsevier Science B.V. All
rights reserved.
4. L.
Alff, S. Kleefisch, B. Welter, K. Sengebusch, S. Meyer, U. Schoop, F.
Herbstritt, A. Marx, R. Gross, M. Naito, and H. Sato
"Symmetry
of the order parameter in hole and electron doped cuprate superconductors"
Physica
C 341, 1659-1662 (2000).
ABSTRACT: It
is well established that the order parameter symmetry in the hole doped
high-temperature superconductors (HTS) is of d-wave type. In contrast, there is
growing experimental evidence for a s-wave type symmetry in the electron doped
cuprate superconductors. We present tunneling spectra and measurements of the
London penetration depth, both supporting strongly the s-wave scenario for the
electron doped HTS [1]. The absence of Andreev bound states in the tunneling
spectra indicates a state without sign change of the pair potential, and the
absence of low energy excitations as revealed by the London penetration depth
measurements suggests a gapped state. Based on these experiments, for the
materials (Nd/Pr)(1.35)Ce0.15CuO4-y an about isotropic s-wave symmetry seems
more likely than a strongly anisotropic s-wave symmetry. For the Nd compound we
observe anomalous low temperature behavior due to the Nd3+ magnetic moments.
5. L.
Alff, S. Meyer, S. Kleefisch, U. Schoop, K. Sengebusch, A. Marx, H. Sato, M.
Naito, and R. Gross
"Low-temperature
anomalies of the superconducting properties of Nd1.85Ce0.15CuO4-y"
Physica
B 284, 999-1000 (2000).
ABSTRACT: We
have measured the temperature dependence of the change Delta lambda(ab)(T) =
lambda(ab)(T) - lambda(ab)(T = 0) of the in-plane London penetration depth
lambda(ab) in the electron-doped cuprate superconductor Nd1.85Ce0.15CoO4-y
(NCCO). An anomalous temperature dependence below about 4 K is observed. In
contrast to the expected monotonous decrease of lambda(ab)(T) With decreasing
temperature, lambda(ab)(T) is found to increase with decreasing temperature
below 4 K resulting in a non-monotonous overall temperature dependence. This
anomalous behavior was found to be absent in analogous measurements performed
on Pr1.85Ce0.15CoO4-y (PCCO). From this, we conclude that the anomalous
behavior of NCCO is caused by the influence of the Nd3+ magnetic moments.
Correcting for the temperature-dependent susceptibility due to the Nd3+
moments, an exponential lambda(ab)(T) dependence is obtained indicating s-wave
pairing in the electron-doped superconductors. (C) 2000 Elsevier Science B.V.
All rights reserved.
6. V.
N. Antonov, H. Takayanagi, F. K. Wilhelm, and A. D. Zaikin
"pi-shifted
magnetoconductance oscillations in mesoscopic superconducting-normal
heterostructures"
Europhys.
Lett. 50 (2), 250-256 (2000).
ABSTRACT:
Interference of proximity-induced superconducting correlations in mesoscopic
metallic rings is sensitive to the magnetic flux Phi inside these rings. This
is the reason for magnetoconductance oscillations in such systems. We detected
experimentally and explained theoretically a novel effect: the phase of these
oscillations can switch between 0 and pi depending on the resistance of
intermetallic interfaces and temperature. The effect is due to a nontrivial
interplay between the proximity-induced enhancement of the local conductivity
and the proximity-induced suppression of the density of states at low energies.
7. H.
Arimoto, T. Saku, Y. Hirayama, and N. Miura
"Anomalous
hysteretic phenomena in cyclotron resonance spectra of GaAs/AlGaAs quantum well
under tilted magnetic fields of short pulse up to 150 T"
Physica
E 6 (1-4), 191-194 (2000).
ABSTRACT: We
observed a new type of hysteresis in cyclotron resonance spectra of two-dimensional
electron gas confined in GaAs/AlGaAs multi quantum wells when we applied high
magnetic fields tilted from the growth direction. Pulsed high magnetic fields
up to 150T were generated by the single turn coil technique. We investigated in
detail the condition for the occurrence of the hysteresis which is a
disagreement between two traces in the up- and down-sweeps of the pulsed
magnetic fields. The dependencies of the hysteresis on the wavelength, sweep
rate of the fields and temperature has led to the conclusion that the
hysteresis is due to inequilibrium states in the up-sweep of tilted magnetic
fields. The relaxation time from inequilibrium to equilibrium states was
revealed to be of the order of microsecond. (C) 2000 Elsevier Science B.V. All
rights reserved.
8. D.
G. Austing, Y. Tokura, S. Tarucha, T. H. Oosterkamp, J. W. Janssen, M. W. S.
Danoesastro, and L. P. Kouwenhoven
"Vertical
quantum dots at high magnetic fields beyond the few-electron limit"
Physica
E-Low-Dimensional Systems & Nanostructures 6
(1-4), 358-363 (2000).
ABSTRACT: We
describe phenomena that can be studied in vertical quantum dot single electron
transistors, Moving from the few-electron to the several- and many-electron
regimes, features in the conductance peaks initially related to spin
polarization evolve with magnetic field. This allows us to first probe the
spin-flip region beyond the last single-particle crossing at low field, and
then the formation and stability of the spin-polarized maximum density droplet
at high field. According to a simple capacitance model, charge redistribution
in the dot at higher magnetic fields is accompanied by abrupt changes in the
area of the droplet. (C) 2000 Elsevier Science B.V. All rights reserved.
9. G.
Bastian
"Comment
on "Critical currents in ballistic two-dimensional InAs-based
superconducting weak links""
Phys.
Rev. B 62 (14), 9840-9841 (2000).
ABSTRACT: In
ballistic Josephson junctions the experimentally observed IV characteristics
deviate from the theoretically predicted behavior. Recently, Heida et al.
[Phys. Rev. B 60, 13 135 (1999)] discussed this problem and offered an
explanation for the discrepancy. Considering this explanation, several
contradictions to the authors' data as wen as to other publications are shown.
10. O.
Benson, J. Kim, H. Kan, and Y. Yamamoto
"Simultaneous
Coulomb blockade for electrons and holes in p-n junctions: observation of
Coulomb staircase and turnstile operation"
Physica
E 8 (1), 5-12 (2000).
ABSTRACT: The
Coulomb blockade effect in a mesoscopic double-barrier p-i-n junction is
reported. The electron and hole injection into the central QW of a p - n
junction is achieved via resonant tunneling. We present a theoretical model
that describes the device operation. When the device is biased with a constant
voltage source the model predicts the observation of Coulomb staircase in the
current-voltage characteristics. When an additional square wave modulation
signal is applied, turnstile operation is achieved. The experimental evidence
for Coulomb staircase effect and turnstile operation is presented. (C) 2000
Elsevier Science B,V. All rights reserved.
11. O.
Benson, C. Santori, M. Pelton, and Y. Yamamoto
"Regulated
and entangled photons from a single quantum dot"
Phys.
Rev. Lett. 84 (11), 2513-2516 (2000).
ABSTRACT: We
propose a new method of generating nonclassical optical field states. The
method uses a semiconductor device, which consists of a single quantum dot as
active medium embedded in a p-i-n junction and surrounded by a microcavity.
Resonant tunneling of electrons and holes into the quantum dot ground states,
together with the Pauli exclusion principle, produce regulated single photons
or regulated pairs of photons. We propose that this device also has the unique
potential to generate pairs of entangled photons at a well-defined repetition
rate.
12. E. V.
Bezuglyi, E. N. Bratus, V. S. Shumeiko, G. Wendin, and H. Takayanagi
"Circuit
theory of multiple Andreev reflections in diffusive SNS junctions: The
incoherent case"
Phys.
Rev. B 62 (21), 14439-14451 (2000).
ABSTRACT: The
incoherent regime of multiple Andreev reflections (MAR) is studied in long
diffusive SNS junctions at applied voltages larger than the Thouless energy.
Incoherent MAR are treated as a transport problem in energy space by means of a
circuit theory for an equivalent electrical network. The current through NS
interfaces is explained in terms of diffusion flows of electrons and holes
through ''tunnel'' and ''Andreev'' resistors. These resistors in diffusive
junctions play roles analogous to the normal and Andreev reflection
coefficients in Octavio-Tinkham-Blonder-Klapwijk theory for ballistic
junctions. The theory is applied to the subharmonic gap structure (SGS); simple
analytical results are obtained for the distribution function and current
spectral density for the limiting cases of resistive and transparent NS
interfaces. In the general case, the exact solution is found in terms of chain
fractions, and the current is calculated numerically. SGS shows qualitatively
different behavior for even and odd subharmonic numbers n = 2 Delta /eV, and
the maximum slopes of the differential resistance correspond to the gap
subharmonics, eV = 2 Delta /n. The influence of inelastic scattering on the
subgap anomalies of the differential resistance is analyzed.
13. V. V.
Borovkov, J. M. Lintuluoto, M. Fujiki, and Y. Inoue
"Temperature
effect on supramolecular chirality induction in bis(zinc porphyrin)"
J.
Am. Chem. Soc. 122 (18), 4403-4407 (2000).
ABSTRACT: The
achiral syn folded conformer (face-to-face) of the ethane-bridged bis(Zn
porphyrin) gradually transforms into the chiral extended anti form in the
presence of enantiopure guest molecules (alcohols or amines) upon lowering the
temperature from 293 to 183 K. The mechanism of the supramolecular chirality
induction is based upon the formation of right- or left-handed screw
diastereomers of the anti form. The split absorption maxima which are caused by
the exciton coupling of the corresponding B transitions match the bisigned
Cotton effects. The amplitude of the CD bands is found to be dependent on the
bulk and ligation strength of the chiral guest, while the sign of the couplets
is observed to be determined by the absolute configuration of the external ligand.
The formation of the screw structure in the anti conformation is also confirmed
by H-1 NMR.
14. D. J.
Bottomley
"Formation
and shape of InAs nanoparticles on GaAs surfaces: Fundamental
thermodynamics"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 39
(7B), 4604-4608 (2000).
ABSTRACT:
Consideration of the heteroepitaxial growth of InAs on GaAs surfaces, and the
substrate orientation-dependent growth mode, has led us to examine the
thermodynamic aspects of heteroepitaxy in general. We argue that the molar
Gibbs free energy G is the appropriate state function for heteroepitaxy, in
contrast to Gibbs's approach of using the Helmholtz free energy, since G alone
guarrantees mathematical continuity in the theory's predictions in the limit of
isotropic stress. An expression for the critical heteroepitaxial strain
required to melt a film is given. We comment that evidence of stress-induced
surface liquid-like phenomena has been present in experiments for over 30
years, but such liquid phase phenomena had no theoretical basis until the
present work. In situ electron microscopy and electron diffraction studies of
heteroepitaxial growth are probably the most favourable techniques for
investigating the proposed liquid phase.
15. A.
Chavez-Pirson, J. Temmyo, and H. Ando
"Pressure-induced
modulation of the confinement in self-organized quantum dots produced and
detected by a near-field optical probe"
Physica
E 7 (3-4), 367-372 (2000).
ABSTRACT:
Near-field optical probing, or nanoprobing, achieves spatial resolution that
surpasses the diffraction limit of light and makes possible the luminescence
imaging and spectroscopy of single quantum dots in dense arrays of dots. We use
optical nanoprobing to study self-organized InGaAs quantum dots grown on (3 1
1)B oriented GaAs substrates. Here, we emphasize a new feature of nanoprobing:
pressure-induced strain modulation near the surface. Operating in near-field
optical excitation-collection mode, the probe makes contact with the surface
and exerts direct pressure whose main effect is a compressive uniaxial strain
under the probe. By adjusting the applied pressure, we modulate the local
strain environment in and around a quantum dot, but still preserve the
capability to capture its near-field luminescence. Nanoprobe pressure effects
modify the confinement potential and radiative emission of single quantum dots,
and the coupling strength between dots. This opens new possibilities for the
study and control of the optical and electronic properties of single- and coupled-quantum
dots. (C) 2000 Elsevier Science B.V. All rights reserved.
16. T.
Dotera and Y. Y. Suzuki
"Polymer
confinement in undulated membrane boxes and tubes"
Phys.
Rev. E 62 (4), 5318-5323 (2000).
ABSTRACT: We
consider quantum particle or Gaussian polymer confinement between two surfaces
and in cylinders with sinusoidal undulations. In terms of the variational
method, we show that the quantum-mechanical wave equations have lower
ground-state energy in these geometries under long wavelength undulations,
where bulges are formed and waves are localized in the bulges. It turns out
correspondingly that Gaussian polymer chains in undulated boxes or tubes
acquire higher entropy than in exactly flat or straight ones. These phenomena
are explained by the uncertainty principle for quantum particles, and by a
polymer confinement rule for Gaussian polymers. If membrane boxes or tubes are
flexible, polymer-induced undulation instability is suggested. We find that the
wavelength of undulations at the threshold of instability for a membrane box is
almost twice the distance between two walls of the box. Surprisingly, we find
that the instability for tubes begins with a shorter wavelength compared to the
"Rayleigh" area-minimizing instability.
17. Z. F.
Ezawa, A. Sawada, K. Muraki, and Y. Hirayama
"Quantum
coherence and skyrmion textures in bilayer quantum Hall systems"
Physica
E 6 (1-4), 640-644 (2000).
ABSTRACT:
Quantum coherence develops spontaneously in bilayer quantum Hall systems when
the Coulomb exchange energy is dominant. We argue that there exists a
distinctive transition between the coherent phase and the resonant phase
because different types of skyrmions are excited in these two phases. (C) 2000
Elsevier Science B.V. All rights reserved.
18. P.
Finnie and Y. Homma
"Stability-instability
transitions in silicon crystal growth"
Phys.
Rev. Lett. 85 (15), 3237-3240 (2000).
ABSTRACT: In
order for a crystal to grow, source atoms must be incorporated into the
underlying lattice. Typically, this process occurs on the surface in one of two
modes: either through island nucleation or through step flow. However, a third,
morphologically unstable growth mode has been predicted. Monitoring the surface
of ultraflat substrates with an in situ scanning electron microscope, we prove
that for the (111) face of silicon there is a transition from stable step flow
to morphological instability and then to island nucleation.
19. P.
Finnie and Y. Homma
"Nucleation
and step flow on ultraflat silicon"
Phys.
Rev. B 62 (12), 8313-8317 (2000).
ABSTRACT:
Step-flow crystal growth is possible on a very large scale on Si(111). The
growth mode changes at the (7x7)-("1x1") phase-transition
temperature. Nucleation of new Steps can be controlled by intentionally
introducing contaminants or particulates. In general, steps bounding small
structures move more quickly than those bounding large structures. Step motion
appears symmetric under time reversal (erosion versus growth) and is similar
under topological inversion (islands versus craters). The observed motion fits
well with the simplest reasonable physical theory.
20. P.
Finnie and Y. Homma
"Motion
of atomic steps on ultraflat Si(111): Constructive collisions"
J.
Vac. Sci. Technol. A-Vac. Surf. Films 18 (4),
1941-1945 (2000).
ABSTRACT: The
motion of atomic steps was studied using ultraflat Si(lll) substrates which
have flat terraces of up to 50 mu m in width separated by monoatomic steps. The
motion is revealed in time lapse movies made by in situ scanning electron
microscopy. When samples are heated to high temperatures (similar to 1000
degrees C) the surface erodes in a step-flow mode: steps retreat in an orderly
fashion, one after the other. Here, steps are forced to collide constructively,
providing a means to probe step interactions. Diffusion theory is used to
explain the collision dynamics, allowing the extraction of physical parameters.
After colliding, double steps continue to move at speeds simply related to the
precursor steps' velocities. (C) 2000 American Vacuum Society.
[S0734-2101(00)03004-9].
21. S. R.
Friberg, T. Mukai, and S. Machida
"Dual
quantum nondemolition measurements via successive soliton collisions"
Phys.
Rev. Lett. 84 (1), 59-62 (2000).
ABSTRACT:
integral(0)(infinity) dse(-s(m2+2D))[I-0(2s)](D) Quantum mechanics allows
quantum nondemolition (QND) variables to be measured without being changed.
This requires QND variables to be initially in an eigenstate and measurement
backaction noise to be directed into conjugate variables. Experimental
demonstrations thus require two measurements: the first to collapse variables
toward an eigenstate and the second to show results identical to the first.
Here, we report results from two successive soliton-collision QND measurements
that optical correlation measurements show to be nearly identical.
22. T.
Fujii, T. Watanabe, and A. Matsuda
"Anisotropy
in the superconducting state and c-axis resistivity of precisely oxygen
controlled Bi2Sr2CaCu2O8+delta a single crystals"
Physica
C 341, 1873-1874 (2000).
ABSTRACT: We
have measured the angle dependence of magneto-resistivity for pure
Bi2Sr2CaCu2O8+delta Single crystals with various oxygen contents. Blatter's
scaling rule was applied to estimate the anisotropy gamma in the
superconducting state. With reducing oxygen content, obtained gamma increases
in proportional to the square root of the rho (c) at just above T-c. These
results can be quantitatively explained by the Lawrence-Doniach model. However,
the obtained gamma has a temperature dependence, which suggests anomalous
effect on the interlayer coupling eta near T-c.
23. M.
Fujiki
"Synthesis
and structure-property-functionality relationship of optically active
polysilanes"
J.
Synth. Org. Chem. Jpn. 58 (12), 1178-1188 (2000).
ABSTRACT:
Chainlike polysilanes, which consist of a linear silicon-catenated backbone and
organic side chains, exhibit unique optical properties due to the silicon sigma
-conjugating electronic structure. Among these polysilanes, it has been
established that rodlike polysilanes bearing a special pair of chiral and/or
achiral alkyl side chains have unique (chir)optical features due to the highly
delocalized silicon sigma electrons associated with very long segment lengths.
The author describes several marked cooperative phenomena of optically active
rodlike polysilane homopolymers and copolymers bearing (S/R)-2-methylbutyl or
(S/R)-3,7-dimethyloctyl chiral side chains by means of UV, circular dichroism
(CD), and fluorescence (FL) spectra and molecular mechanics calculation.
24. M.
Fujiki
"Helix
magic. Thermo-driven chiroptical switching and screw-sense inversion of
flexible rod helical polysilylenes"
J.
Am. Chem. Soc. 122 (14), 3336-3343 (2000).
ABSTRACT: An
ideal optically active helical chromophoric polymer comprising a flexible
rodlike silicon main chain and enantiopure alkyl side chains,
poly{(S)-3,7-dimethyloctyl-3-methylbutylene}, underwent a thermo-driven
helix-helix transition at -20 degrees C in isooctane. The transition
characteristics. including transition temperature, transition width, the
population of right- and left-handed helical motifs, global shape, and
screw-pitch, were to be characterized quantitatively by spectroscopically
analyzing circular dichroism (CD) and UV absorption characteristics. This is
based on the unique property of the rodlike polymer in which the CD band
completely matches the corresponding UV band profile at all temperatures.
Moreover, fine controlling the contents and chirality of an additional chiral
silylene unit incorporated in the copolymers allows free manipulation of the
transition temperature in the range from -64 to +79 degrees C. Molecular
mechanics calculation showed remarkable differences in the potential energy
curve of the main chain torsion angle between flexible and rigid rodlike
polysilylenes. These results and knowledge gained should assist in designing
and controlling new types of helix-helix transition polymers directed to
diverse screw-sense related properties and applications.
25. T.
Fujisawa and Y. Hirayama
"Transmission
type RF single electron transistor operation of a semiconductor quantum
dot"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 39
(4B), 2338-2340 (2000).
ABSTRACT: A
single electron transistor is a highly sensitive electrometer, and can be
operated at a high speed using the radio-frequency single electron transistor
(RF-SET) technique. In this paper, we propose a modified RF-SET technique,
which measures the transmission of the RF signal. It has some advantages, such
as simpler circuits and clear frequency resonance as compared with the
reflection measurement by RF-SET. We have tested the transmission-type RF-SET
operation for a quantum dot in an AlGaAs/GaAs heterostructure.
26. T.
Fujisawa and Y. Hirayama
"Charge
noise analysis of an AlGaAs/GaAs quantum dot using transmission-type
radio-frequency single-electron transistor technique"
Appl.
Phys. Lett. 77 (4), 543-545 (2000).
ABSTRACT:
Radio-frequency (rf)-operated single-electron transistors (SETs) are high-sensitivity,
fast-response electrometers, which are valuable for developing new insights
into single-charge dynamics. We investigate high-frequency (up to 1 MHz) charge
noise in an AlGaAs/GaAs quantum dot using a transmission-type rf SET technique.
The electron capture and emission kinetics on a trap in the vicinity of the
quantum dot are dominated by a Poisson process. The maximum bandwidth for
measuring single trapping events is about 1 MHz, which is the same as that
required for observing single-electron tunneling oscillations in a measurable
current (similar to 0.1 pA). (C) 2000 American Institute of Physics.
[S0003-6951(00)00130-3].
27. T.
Fujisawa, W. G. van der Wiel, and L. P. Kouwenhoven
"Inelastic
tunneling in a double quantum dot coupled to a bosonic environment"
Physica
E 7 (3-4), 413-419 (2000).
ABSTRACT:
Coupling a quantum system to a bosonic environment always give rise to
inelastic processes, which reduce the coherency of the system. We measure
energy-dependent rates for inelastic tunneling processes in a fully
controllable two-level system of a double quantum dot. The emission and
absorption rates are well reproduced by Einstein's coefficients, which relate
to the spontaneous emission rate. The inelastic tunneling rate can be comparable
to the elastic tunneling rate if the boson occupation number becomes large. In
the specific semiconductor double dot, the energy dependence of the inelastic
rate suggests that acoustic phonons are coupled to the double dot
piezoelectrically. (C) 2000 Elsevier Science B.V. All rights reserved.
28. K.
Furukawa and K. Ebata
"Preparation
and single molecule structure of electroactive polysilane end-grafted on a
crystalline silicon surface"
Appl.
Phys. Lett. 77 (26), 4289-4291 (2000).
ABSTRACT:
Electrically active polysilanes of poly(methylphenylsilane) (PMPS) and
poly[bis(p-n-butylphenyl)silane] (PBPS), which are, respectively, known as a
good hole transporting material and a near-ultraviolet electroluminescent
material, are end-grafted directly on a crystalline silicon surface. The single
polysilane molecules are clearly distinguished one from the other on the
surface by means of atomic force microscopy observations. End-grafted single
molecules of PMPS are observed as dots while end-grafted PBPS appear as worms
extending for more than 100 nm on the crystalline silicon surface. (C) 2000
American Institute of Physics. [S0003- 6951(00)03052-7].
29. K.
Furukawa, K. Ebata, and M. Fujiki
"One-dimensional
silicon chain architecture: Molecular dot, rope, octopus, and toroid"
Adv.
Mater. 12 (14), 1033-1036 (2000).
ABSTRACT:
30. J. R.
Goldman, T. D. Ladd, F. Yamaguchi, and Y. Yamamoto
"Magnet
designs for a crystal-lattice quantum computer"
Appl.
Phys. A-Mater. Sci. Process. 71 (1), 11-17 (2000).
ABSTRACT: A
quantum computer using nuclear spins in a crystal lattice requires a method for
addressing individual quantum bits. This identification can be achieved with a
spatially varying magnetic field. Spins at different lattice sites can have
distinguishable Zeeman frequencies allowing initialization, logic operations,
and measurements to be performed through radio frequency (rf) pulse techniques.
Here, we present magnet designs that have gradients between 1 and 20 T/mu m,
which are necessary to realize quantum computation with particular crystals.
PACS: 03.67.Lx; 76.60.Pc; 85.70.w.
31. H.
Gotoh, H. Ando, T. Sogawa, H. Kamada, T. Kagawa, and H. Iwamura
"Effect
of electron-hole interaction on electron spin relaxation in GaAs/AlGaAs quantum
wells at room temperature"
J.
Appl. Phys. 87 (7), 3394-3398 (2000).
ABSTRACT: We
investigated electron spin relaxation with respect to the spatial electron-hole
separation in GaAs/AlGaAs quantum wells at room temperature. The polarization
dependent time-resolved photoluminescence method was used to measure the
electron spin relaxation time by applying an electric field perpendicular to
the quantum wells. The spin relaxation time had a strong electric field
dependence and largely increased with an increase in the spatial electron-hole
separation. These results cannot be explained by only the D'yakonov-Perel
process, which has often been considered the cause of spin relaxation. We
discuss the possible mechanisms that cause the spin relaxation by taking into
account the electron-hole exchange interaction. (C) 2000 American Institute of
Physics. [S0021-8979(00)04207-9].
32. H.
Gotoh, H. Kamada, H. Ando, and J. Temmyo
"Lateral
electric-field effects on excitonic photoemissions in InGaAs quantum
disks"
Appl.
Phys. Lett. 76 (7), 867-869 (2000).
ABSTRACT:
Electric-field effects on excitons in zero-dimensional InGaAs quantum disks
have been examined at low temperature. Photoluminescence from a single isolated
disk was measured under the application of a lateral electric field by using
the microphotoluminescence technique. A redshift of sharp excitonic
luminescence and a decrease in its intensity under increasing electric field
were observed. These were found to distinctively depend on the lateral extent
of the disks: these were much more prominent in the larger disk. The exciton
luminescence was found to be highly polarized along the direction of the field
in the larger disk. (C) 2000 American Institute of Physics.
[S0003-6951(00)00207-2].
33. D. M.
Halliday
"Weak,
stochastic temporal correlation of large-scale synaptic input is a major
determinant of neuronal bandwidth"
Neural
Comput. 12 (3), 693-707 (2000).
ABSTRACT: We
determine the bandwidth of a model neurone to large-scale synaptic input by
assessing the frequency response between the outputs of a two-cell simulation
that share a percentage of the total synaptic input. For temporally
uncorrelated inputs, a large percentage of common inputs are required before
the output discharges of the two cells exhibit significant correlation. In
contrast, a small percentage (5%) of the total synaptic input that involves
stochastic spike trains that are weakly correlated over a broad range of
frequencies exert a clear influence on the output discharge of both cells over
this range of frequencies. Inputs that are weakly correlated at a single
frequency induce correlation between the output discharges only at the
frequency of correlation. The strength of temporal correlation required is
sufficiently weak that analysis of a sample pair of input spike trains could
fail to reveal the presence of correlated input. Weak temporal correlation
between inputs is therefore a major determinant of the transmission to the
output discharge of frequencies present in the spike discharges of presynaptic
inputs, and therefore of neural bandwidth.
34. O.
Hanaizumi, K. Miura, M. Saito, T. Sato, S. Kawakami, E. Kuramochi, and S. Oku
"Frontiers
related with automatic shaping of photonic crystals"
IEICE
Trans. Electron. E83C (6), 912-919 (2000).
ABSTRACT:
Photonic crystals have optical properties characterized by photonic bandgap,
large anisotropy and high dispersion, which can be applied to Various optical
devices. We have proposed an autocloning method for fabricating 2D or 3D
photonic crystals and are developing novel structures and functions in photonic
crystals. The autocloning is an easy process based on the combination of
sputter deposition and sputter etching and is suitable for industry. We have
already demonstrated devices or functions such as polarization splitters and
surface-normal waveguides. In this paper, we describe our latest work on
photonic crystals utilizing the autocloning technology. Phase plates and
polarization selective gratings for optical pick-ups are demonstrated utilizing
TiO2/SiO2 photonic crystals. The technology to introduce CdS into 3D photonic
crystals is also developed and photoluminescence from the introduced CdS is
observed, which is the first step to realize luminescent devices with 3D
confinement or high polarization controllability.
35. J. B.
Hannon, H. Hibino, N. C. Bartelt, B. S. Swartzentruber, T. Ogino, and G. L.
Kellogg
"Dynamics
of the silicon (111) surface phase transition"
Nature 405
(6786), 552-554 (2000).
ABSTRACT: The
manner in which phase transformations occur in solids determines important
structural and physical properties of many materials. The main problem in
characterizing the kinetic processes that occur during phase transformations is
the difficulty of observing directly, in real time, the growth of one phase at
the expense of another. Here we use low-energy electron microscopy to study the
real-time kinetics of a phase transformation confined to the silicon (111)
surface. We show that the transformation is governed by the rate at which material
is exchanged between the first layer of the crystal and the surface. In bulk
phase transformations. the dynamics are usually governed either by the rate of
diffusion of material to the phase boundaries or by the structural
rearrangement of atoms at the phase boundary(1). The kinetic process that we
have identified here has no bulk analogue and leads to domain dynamics that are
qualitatively different from these expected for bulk systems.
36. K.
Hashio, M. Tatsumi, H. Kato, and K. Kinoshita
"Directional
solidification of InxGa1-xAs"
J.
Cryst. Growth 210 (4), 471-477 (2000).
ABSTRACT: We
have investigated a constitutional supercooling and segregation phenomena in
InxGa1-xAs crystals unidirectionally solidified in a Vertical system. The
constitutional supercooling generates characteristic fluctuations of
composition along the growth direction and this can be explained by a free
nucleation ahead from the growth interface. The macroscopic compositional
profiles of the grown crystals suggest that a transport of solute is mainly
dominated by the diffusion. Such a growth mode is partly attributed to the
difference in density between InAs and GaAs, (C) 2000 Elsevier Science B.V. All
rights reserved.
37. N.
Hatakenaka, H. Takayanagi, Y. Kasai, and S. Tanda
"Double
sine-Gordon fluxons in isolated long Josephson junctions"
Physica
B 284, 563-564 (2000).
ABSTRACT: A
quantum flux, a 2 pi fluxon, described by a sine-Gordon equation is an
elementary excitation in long Josephson junctions. We investigated the fluxon
dynamics in isolated long Josephson junctions. In such isolated systems, the
total number of Cooper pairs is conserved, so the fluxon dynamics map change.
We found that the fluxons obey a double sine-Gordon (DSG) equation based on
this change in the Josephson acceleration relation, i.e., the voltage-phase
difference relation. It should be possible to confirm the existence of DSG
fluxons by detecting the relative oscillations of two pi fluxons. (C) 2000
Elsevier Science B.V. All rights reserved.
38. K.
Hayashi, T. Horiuchi, R. Kurita, K. Torimitsu, and O. Niwa
"Real-time
electrochemical imaging using an individually addressable multi-channel
electrode"
Biosens.
Bioelectron. 15 (9-10), 523-529 (2000).
ABSTRACT: We
developed a real-time electrochemical imaging method that uses a multiple
enzyme-modified microelectrode. The method will enable the investigation of the
functions of biological materials and cells. To test its effectiveness, we
imaged the two-dimensional concentration distribution for hydrogen peroxide and
L-glutamate in a standard solution. The multiple electrode consists of an 8 x 8
array of 30 x 30 mum(2) carbon micro electrode. Each electrode was connected to
a 64-channel potentiostat that could apply a potential to all electrodes at the
same time. The multiple electrode was coated with an Os-polyvinylpyridine based
polymer (Os-gel) containing horse radish peroxidase (HRP) to detect hydrogen
peroxide, which is a very common product of oxidase enzyme. When measuring
glutamate, which is a well-known neurotransmitter in the mammalian central
nerve system, we modified the electrode with a bilayer of Os-gel-HRP and GluOx.
The detection limit of our method was 1 muM and images of the glutamate
concentration-distribution changes induced by local injection of glutamate
through microcapillary were obtained in real time. (C) 2000 Elsevier Science
S.A. All rights reserved.
39. H.
Hibino, T. Kawamura, and T. Ogino
"RHEED
analysis of twinned homoepitaxial layers grown on Si(111)root 3x root 3-B"
Thin
Solid Films 369 (1-2), 5-9 (2000).
ABSTRACT:
Homoepitaxial Si layers grown on Si(111)root 3 X root 3-B have an orientation
rotated by 180 degrees with respect to the substrate, i.e. a twinned
orientation. The growth of the twinned epitaxial layers is monitored in situ
using reflection high-energy electron diffraction (RHEED). RHEED intensities
change quite sensitively with respect to the thickness of the twinned layers
even at the thickness of two bilayers. After six-bilayer growth, the RHEED
pattern is almost the same as the pattern diffracted from the substrate in the
incident azimuth rotated by 180 degrees. Calculations of RHEED intensities
based on the multiple scattering theory reproduce well the measured
intensities. (C) 2000 Published by Elsevier Science S.A. All rights reserved.
40. H.
Hibino and T. Ogino
"Si
twinning superlattice: Growth of new single crystal Si"
Surf.
Rev. Lett. 7 (5-6), 631-635 (2000).
ABSTRACT: Si
twinning superlattices are grown on Si(111)(root3 x root3)-B by the repeated
growth of Si layers with a unit thickness and postgrowth annealing. In order to
determine the growth conditions of the Si twinning superlattice, it is
essential to measure the crystallographic orientations in the surface regions
during growth, Reflection high-energy electron diffraction (RHEED) is very
sensitive to the surface orientation. Using the technique to estimate the
fraction of the twinned layers in the grown layers by RHEED, we investigate the
growth process and thermal stability of the twinned epitaxial layers. The
growth of the twinning superlattices is monitored by the oscillation of the
twinned layer fraction as a function of the thickness.
41. T.
Higashino, J. Osaka, K. Tanahashi, M. Kikuchi, Y. Kawamura, N. Inoue, and Y.
Homma
"The
measurement of work function on GaAs (001) surface during MBE growth by
scanning electron microscopy"
J.
Cryst. Growth 209 (2-3), 431-434 (2000).
ABSTRACT:
Secondary electron (SE) intensity was measured in situ during Ga supply on the
molecular beam epitaxy (MBE) grown GaAs (0 0 1) surface using scanning electron
microsope-MBE hybrid system. SE intensity changed in the opposite way to the
reported work function change and the correspondence was excellent. This is
promising for in situ, nondestructive determination of local work function
during MBE growth or nanometer device process in vacuum. (C) 2000 Elsevier
Science B.V. All rights reserved.
42. Y. Homma
and N. Aizawa
"Electric-current-induced
step bunching on Si(111)"
Phys.
Rev. B 62 (12), 8323-8329 (2000).
ABSTRACT: We
experimentally investigated step bunching induced by direct current on vicinal
Si(111)"1x1" surfaces using scanning electron microscopy and atomic
force microscopy. The scaling relation between the average step spacing l(b)
and the number of steps N in a bunch, l(b)similar to N-alpha, was determined
for four step-bunching temperature regimes above the 7x7-"1x1"
transition temperature. The step-bunching rate and scaling exponent differ
between neighboring step-bunching regimes. The exponent alpha is 0.7 for the
two regimes where the step-down current induces step bunching (860-960 and
1210-1300 degrees C), and 0.6 for the two regimes where the step-up current
induces step bunching (1060-1190 and >1320 degrees C). The number of single
steps on terraces also differs in each of the four temperature regimes. For
temperatures higher than 1280 degrees C, the prefactor of the scaling relation
increases, indicating an increase in step-step repulsion. The scaling exponents
obtained agree reasonably well with those predicted by theoretical models.
However, they give unrealistic values for the effective charges of adatoms for
step-up-current-induced step bunching when the ''transparent'' step model is
used.
43. Y.
Homma, P. Finnie, and T. Ogino
"Ultrahigh
vacuum scanning electron/tunneling combined microscope system"
in
Microbeam Analysis 2000, Proceedings, Institute Of Physics Conference
Series Vol. 165 (Iop Publishing Ltd, Bristol, 2000), pp. 375-376.
ABSTRACT:
44. Y.
Homma, P. Finnie, and T. Ogino
"Control
of island formation on silicon surfaces using ultra-high-vacuum scanning
electron microscopy"
J.
Electron Microsc. 49 (2), 225-229 (2000).
ABSTRACT: In
situ scanning electron microscopy has been used to control Au island formation
on a patterned Si(111) surface with a periodic array of atomic-step bunches and
holes. Liquid phase Au-Si islands were observed to redistribute on the
patterned surface by annealing. The islands accumulate at a particular position
of the step bunch in each pattern unit. This phenomenon is interpreted in terms
of the energetic stability of a droplet on a patterned surface.
45. Y.
Homma, H. Hibino, Y. Kunii, and T. Ogino
"Transformation
of surface structures on vicinal Si(111) during heating"
Surf.
Sci. 445 (2-3), 327-334 (2000).
ABSTRACT: We
investigated transformation processes of holes and hillocks on vicinal Si(1 1
1) surfaces during annealing at around 1200 degrees C using ultra-high-vacuum
scanning electron microscopy. A hole and a hillock decay symmetrically with one
another: their shapes are complementary, and the decay rate is almost the same
except during the final stage, where hillocks decay faster than holes. Flat
surfaces appear both at the bottom of the hole and at the top of the hillock
due to layer-by-layer decay. As a result of transformation, regularly arranged
atomic-step bunches are formed in both cases. The electric current used for
sample heating greatly affects the final shape of step bunches. The current
direction that induces step bunching on a flat surface creates straighter step
bunches than the opposite direction. For holes larger than the adatom diffusion
length, step-flow sublimation becomes the dominant process instead of
layer-by-layer filling-in of the bottom terrace, which is the dominant process
for holes smaller than the adatom diffusion length. (C) 2000 Elsevier Science
B.V. All rights reserved.
46. T.
Horiuchi, O. Niwa, and N. Hatakenaka
"Electrochemiluminescence
at a microelectrode in a microscale fluidic system"
Electroanalysis 12
(9), 672-676 (2000).
ABSTRACT: We
describe the real-time visualization of electrochemiluminescence (ECL) in a
microscale region using an interdigitated array electrode (IDA) in a thin layer
flow cell. We studied the ECL reaction, which is based on the annihilation of
cations and anions of 9,10-diphenylanthracene at the IDA, from the spatial and
temporal emission patterns in the thin layer. We observed that the ECL emission
region moved from the root of the band array to its center and the emission
time was limited when the dye solution was static. We found that two kinds of
microscale-width solution stream formed spontaneously and were arranged
alternately when the solution was under the laminar flow conditions at a
specific flow rate. The two streams were composed of different radical
components.
47. S.
Hoshino, K. Ebata, and K. Furukawa
"Near-ultraviolet
electroluminescent performance of polysilane-based light-emitting diodes with a
double-layer structure"
J.
Appl. Phys. 87 (4), 1968-1973 (2000).
ABSTRACT: We
fabricated double-layer light-emitting diodes (LEDs) by utilizing
poly[bis(p-nbutylphenyl)silane] (PBPS) and oxadiazole derivatives, and
investigated their basic LED characteristics. The near-ultraviolet
electroluminescence (EL) performance, such as the EL threshold electric field
and the current density, depended on the oxadiazole derivatives used as the
electron transport materials as well as the components of the EL emission. We
observed better EL performance where the EL external quantum efficiency in a
double-layer LED with a
2-(4'-tert-butylphenyl)-5-(4'-biphenyl)-1,3,4-oxadiazole based electron
transport layer was twice that of a PBPS single-layer LED. By contrast, we
observed a worse EL threshold electric field and current density when we used
2,5-bis(1-naphthyl)-1,3,4-oxadiazole as an electron transport material. The
reason for the difference in the EL performance was revealed by investigating
the charge carrier injection and transport dynamics of the two LEDs. (C) 2000
American Institute of Physics. [S0021-8979(00)01204-4].
48. S.
Hoshino, K. Furukawa, K. Ebata, I. Breyl, and H. Suzuki
"Molecular
weight dependence of the conformational phase transition and
electroluminescence of diarylpolysilane diodes"
J.
Appl. Phys. 88 (6), 3408-3413 (2000).
ABSTRACT: We
investigated the molecular weight dependence of the conformational phase
transition behavior of thin films of poly[bis(p-n-butylphenyl)silane] (PBPS),
which is a near-ultraviolet (NUV) electroluminescence (EL) material for
polysilane-based polymer light-emitting diodes (LEDs). A low molecular weight
PBPS with efficient NUV EL exhibited a phase transition from a disordered to an
ordered backbone conformation when we increased the temperature. By contrast,
the opposite transition behavior was observed for a high molecular weight PBPS.
The photoluminescence (PL) quantum yield of the PBPS films changed in
association with the thermal phase transition behavior; the PL quantum yield of
the low molecular weight PBPS was improved by increasing the temperature,
whereas that of the high molecular weight polymer deteriorated. The time
dependence of the EL investigation suggests that, although the EL intensity
continued to increase for the first few hours, insufficient Joule heat was
generated to induce a phase transition in the entire PBPS layer of an LED made
of the low molecular weight PBPS during continuous operation. We conclude that
the conformational phase transition was not a key factor as regards efficient
NUV EL generation, but may have occurred at the molecules in contact with the
external electrodes of the LED, and may have been partially responsible for the
improvement in the carrier injection efficiency of the external electrodes. (C)
2000 American Institute of Physics. [S0021-8979(00)01019-7].
49. S.
Hoshino, K. Furukawa, K. Ebata, C. H. Yuan, and H. Suzuki
"Molecular
weight dependent electroluminescence of silicon polymer near-ultraviolet
light-emitting diodes"
J.
Appl. Phys. 88 (5), 2892-2897 (2000).
ABSTRACT: We
investigated the electroluminescence (EL) of single-layer near-ultraviolet
(NUV) light-emitting diodes (LEDs) made from poly[bis(p-n-butylphenyl)silane]
(PBPS) with three different molecular weights (MWs). Although the NUV EL
spectra of the three LEDs exhibited no noticeable differences, we observed a
marked MW dependence on such aspects of the operating performance as the EL
external quantum efficiency, EL threshold current density and electric field,
which were improved as the MW of PBPS decreased. The MW dependence of the hole
transport behavior suggested that the MW decrease promoted positive space
charge formation in the PBPS layer during LED operation. We attributed the
origin of the MW dependence of the LED performance to this positive space
charge formation, which played an important role in improving the electron-hole
supply balance from the external electrodes of the LED. (C) 2000 American
Institute of Physics. [S0021- 8979(00)06717-7].
50. C. M.
Hu, J. Nitta, T. Akazaki, and H. Takayanagi
"Evidence
of the Coulomb gap observed in an InAs inserted In0.53Ga0.47As/In0.52Al0.48As
heterostructure"
Physica
E 7 (3-4), 795-798 (2000).
ABSTRACT: We
report studies of the in-plane magneto-transport properties of a 2DEG in an
InAs inserted InGaAs/InAlAs heterostructure with a DC bias voltage. Temperature
dependent zero-bias reduction of the longitudinal resistance was observed when
high magnetic field is applied along the sample growth direction. We interpret
the observed resistance reduction as the result of a Coulomb gap existing at
the Fermi level of the 2DEG. (C) 2000 Elsevier Science B.V. All rights
reserved.
51. C. M.
Hu, J. Nitta, T. Akazaki, H. Takayanagi, J. Osaka, P. Pfeffer, and W. Zawadzki
"Observation
of the zero-field spin splitting of the second subband in an inverted
In0.53Ga0.47As/In0.52Al0.48As heterostructure"
Physica
E-Low-Dimensional Systems & Nanostructures 6
(1-4), 767-770 (2000).
ABSTRACT: A
gated inverted In0.52Al0.48As/In0.53Ga0.47As/In0.52Al0.48As quantum well is
studied via magneto transport. By analysing the gate-voltage-dependent beating:
pattern observed in the Shubnikov-de Haas oscillation, we determine the gate
voltage (or electron concentration) dependence of the spin-orbit coupling
parameter alpha, Our experimental data and their analysis show that the band
nonparbolicity effect cannot be neglected. For electron concentrations above 2
x 10(12) cm(-2), it causes a reduction of alpha up to 25%. We report for the:
first time the alpha value for the second subband. (C) 2000 Elsevier Science
B.V. All rights reserved.
52. R. P.
Huebener, O. M. Stoll, and M. Naito
"Vortex
core physics in the cuprate superconductor Nd2-xCexCuOy"
Physica
B 280 (1-4), 237-238 (2000).
ABSTRACT:
Flux-how voltage steps and negative differential resistivity in the cuprate
Nd2-xCexCuOy are explained in terms of subbands between the Fermi energy and
the energy gap affecting the quasiparticle dynamics. (C) 2000 Elsevier Science
B.V. All rights reserved.
53. R. P.
Huebener, O. M. Stoll, A. Wehner, and M. Naito
"Flux-flow
resistance in the cuprate superconductor Nd2-xCexCuOy: subbands, Bloch
oscillations, and Zener breakdown"
Physica
C 338 (3), 221-226 (2000).
ABSTRACT: At
intermediate magnetic fields B-c1 much less than B < B-c2 and at
temperatures T much less than T-c, the flux-flow resistance of the cuprate
superconductor Nd2-xCexCuOy (NCCO) displays two intrinsic steps as a function
of the electric field. In explaining this strongly nonlinear behavior, we
propose a scenario based on two subbands between the Fermi energy and the gap
energy, leading to Bloch oscillations and Zener breakdown for the quasiparticle
dynamics. The subbands originate from the Andreev bound states in the core of
an isolated vortex due to the interaction between the vortices. The proposed
scenario appears to explain in particular the observed magnetic field and
temperature dependence of the flux-flow resistance steps. (C) 2000 Elsevier
Science B.V. All rights reserved.
54. R. P.
Huebener, O. M. Stoll, A. Wehner, and M. Naito
"Nonlinear
vortex dynamics in the cuprate superconductor Nd2-xCexCuOy"
Physica
C 332 (1-4), 187-192 (2000).
ABSTRACT: At
T much less than T-c, the flux-flow voltage in the cuprate superconductor
Nd2-xCexCuOy shows an intrinsic step structure that leads to negative
differential resistivity. This is explained in terms of subbands between the
Fermi energy and the gap energy affecting the quasiparticle dynamics. In the
electric field generated by current-induced vortex motion, the quasiparticle
energy can be shifted to the upper band edge, resulting in Bragg reflection and
Bloch oscillations. The subbands originate from the Andreev-bound states in the
core of an isolated vortex, because of the interaction between vortices. (C)
2000 Elsevier Science B.V. All rights reserved.
55. K. Inoue
"Penalty-free
operation of a DFB-LD in a state of coherence collapse and its application to
interferometric noise reduction"
IEICE
Trans. Commun. E83B (12), 2702-2704 (2000).
ABSTRACT:
When a single-mode LD is subjected to distant reflection, relative intensity
noise and the width of the optical spectrum are drastically increased. This
phenomenon is known as 'coherence collapse.' This letter demonstrates that
penalty-free operation is possible at 2.5 Gbit/s even when a DFB-LD is in a
state of coherence collapse. In addition, an LD in a state of coherence
collapse is applied to a situation where signal light suffers from
interferometric crosstalk. The results show that the LD reduces the influence
of interferometric noise because of its wide spectral width.
56. K. Inoue
"Optical
level equalisation based on gain saturation in fibre optical parametric
amplifier"
Electron.
Lett. 36 (12), 1016-1017 (2000).
ABSTRACT:
Optical level equalisation operation based on gain saturation in an optical
fibre parametric amplifier is reported. The signal output has been measured as
a function of the signal input in a fibre parametric amplifier, with the result
that the signal gain saturates as the input power increases and the output
Fewer reached a maximum value at a particular input level. Utilising this gain
saturation property, optical level equalisation has been demonstrated.
57. S.
Ishihara
"Frontiers
of semiconductor technologies in the 21st century"
Ntt
Rev. 12 (6), 40-43 (2000).
ABSTRACT:
Advances in information technology mean new functionality is required in
semiconductor devices. Devices that can work in severe environments, such as
high temperatures, are also becoming important as the application fields of
semiconductor devices expand. At NTT Basic Research Laboratories, we are
investigating a novel device fabrication process based on control of the atomic
structures on silicon surfaces and new materials for environmentally-hardened
devices.
58. S.
Ishihara
"Quantum
physics for future communication technologies - Towards quantum information
processing"
Ntt
Rev. 12 (1), 8-11 (2000).
ABSTRACT: NTT
Basic Research Laboratories are devoted to discovering new principles and
creating new devices that will have major impacts on 21st century
communications. As examples of such research, in this special issue, we will
introduce a single electron device with ultralow power consumption, a quantum
computer that will be able to quickly solve problems that are all but
unsolvable by present computers, and quantum cryptography that guarantees
tamper-free communications.
59. T.
Ishii, T. Tamamura, and K. Shigehara
"Fullerene-derivative
nanocomposite resist for nanometer pattern fabrication"
Jpn.
J. Appl. Phys. Part 2 - Lett. 39 (10B), L1068-L1070 (2000).
ABSTRACT: A
nanocomposite resist system that incorporates a fullerene derivative into a
conventional positive-type electron-beam resist, ZEP520, is examined. Because
of the enhanced solubility of the derivative, the system exhibits a minimal
decrease of sensitivity even at an incorporation content of 50 wt% and enables
the fabrication of 50 nm patterns with a line dose of 0.39 nC/cm. At higher
contents, however, the derivative is not as effective as fullerene C-60 or C-70
in improving dry-etching resistance because of the aggregation of the
derivative molecules, which is probably due to the uniqueness of the derivative
used and will be avoided by appropriate molecular design.
60. Y.
Jimbo, A. Kawana, P. Parodi, and V. Torre
"The
dynamics of a neuronal culture of dissociated cortical neurons of neonatal
rats"
Biol.
Cybern. 83 (1), 1-20 (2000).
ABSTRACT:
Neuronal networks of dissociated cortical neurons from neonatal rats were
cultured over a multielectrode dish with 64 active sites, which were used both
for recording the electrical activity and for stimulation. After about 4 weeks
of culture, a dense network of neurons had developed and their electrical
activity was studied. When a brief voltage pulse was applied to one
extracellular electrode, a clear electrical response was evoked over almost the
entire network. When a strong voltage pulse was used, the response was composed
of an early phase, terminating within 25 ms, and a late phase which could last
several hundreds of milliseconds. Action potentials evoked during the early phase
occurred with a precise timing with a small jitter and the electrical activity
initiated by a localized stimulation diffused significantly over the network.
In contrast, the late phase was characterized by the occurrence of clusters of
electrical activity with significant spatio-temporal fluctuations. The late
phase was suppressed by adding small amounts of D(-)-2-amino-5-phosphonovaleric
acid to the extracellular medium, or by increasing the amount of extracellular
Mg2+. The electrical activity of the network was substantially increased by the
addition of bicuculline to the extracellular medium. The results presented here
show that the neuronal network may exist in two different dynamical states: one
state in which the neuronal network behaves as a non-chaotic deterministic
system and another state where the system exhibits large spatio-temporal
fluctuations, characteristic of stochastic or chaotic systems.
61. Y. Jimbo
and H. P. C. Robinson
"Propagation
of spontaneous synchronized activity in cortical slice cultures recorded by
planar electrode arrays"
Bioelectrochemistry 51
(2), 107-115 (2000).
ABSTRACT: The
spatial propagation of synchronized activity in cortical slice cultures was
characterized by multi-site extracellular recording. Spontaneous activity was
studied in normal culture medium, and in bicuculline- or kainic acid-containing
media. A common feature in all these conditions was that activity was generated
first in superficial layers (i.e., layer I/II) before spreading over the whole
area of the slice. In culture medium or bicuculline-containing medium, the
initiation site of the activity was not constant and showed a large variety of
patterns of horizontal propagation. Kainic acid induced epileptiform activity,
consisting of intense initial bursts followed by repetitive after-discharges.
Though the patterns of spatial propagation of the bursts were variable as in
the other conditions, the after-discharges followed a constant path.
Cross-correlation analysis indicated that the network moved in a graded fashion
to a steady state during the sequence of after-discharges. (C) 2000 Elsevier
Science S.A. All rights reserved.
62. M. R.
Junnarkar and N. Uesugi
"Near
two-photon resonance short pulse compression in atomic noble gases"
Opt.
Commun. 175 (4-6), 447-459 (2000).
ABSTRACT: We
simulate a pulse compression mechanism based on a near two-photon resonance
(NTPR) transition contribution to the nonlinear refractive index of atomic
Noble gas filled hollow waveguides, The negative refractive index contribution
in the normal dispersive gas waveguide plays a similar role as in the case of
soliton compression with positive Kerr nonlinearity and anomalous dispersion in
optical fibers. The sell-pulse compression to similar to 15 fs can be achieved
at moderate peak powers (similar to MW) for 100 fs pulses in the spectral range
100-245 nm. We present simulated data concerning pulse and spectral shapes for
xenon as a case study. The total throughput of the propagated pulse energy is
> 90%, mostly determined by the linear attenuation of the hollow waveguide
propagation mode while two-photon absorption and the corresponding enhanced
three-photon photo-ionization does not significantly reduce the pulse energy.
(C) 2000 Elsevier Science B.V. All rights reserved.
63. H.
Kageshima, K. Shiraishi, H. Ikeda, S. Zaima, and Y. Yasuda
"Selectivity
for O-adsorption position on dihydride Si(100) surfaces"
Appl.
Surf. Sci. 159, 14-18 (2000).
ABSTRACT: The
physics behind the selectivity for the: O adsorption position on dihydride
Si(100) surfaces is studied using HREELS and first-principles calculation. It
is known that on dihydride Si(100) surfaces below 300 degrees C the formed
Si-O-Si bonds do not jointly own any surface Si atoms when the O coverage is
smaller than 80% of the number of outermost surface Si atoms. According to the
present study, the selectivity is not governed by the electronic states near
the Fermi energy at all. Instead, it is governed only by the energetics, and
can be explained in terms of the strain induced by the adsorption itself. (C)
2000 Elsevier Science B.V. All rights reserved.
64. H.
Kageshima, A. Taguchi, and K. Wada
"Theoretical
investigation of nitrogen-doping effect on vacancy aggregation processes in
Si"
Appl.
Phys. Lett. 76 (25), 3718-3720 (2000).
ABSTRACT: The
nitrogen-doping effect on vacancy aggregation in Si is studied by comparing
total energies of various complexes of nitrogen atoms and Si vacancies in terms
of first-principles calculations. Two nitrogen atoms are found to form a stable
complex with two Si vacancies, strongly suggesting that a supersaturation of
"isolated" Si vacancies in growth cooling can be suppressed. The
delayed void formation observed in N-doped Czochralski Si indeed supports this
suggestion. (C) 2000 American Institute of Physics. [S0003-6951(00)03125-9].
65. H.
Kamada, H. Ando, T. Takagahara, J. Temmyo, and T. Tamamura
"Spectroscopies
of exciton and biexciton in InGaAs quantum disk"
J.
Lumines. 87-9, 46-50 (2000).
ABSTRACT:
Exciton in isolated InxGa1-xAs quantum disk was studied by probing single-dot
photoluminescence. Each of the excitonic emission was found to be excited via a
number of sharp-excited state resonances, thereby the discrete density of state
and long-lived phase coherence of the states were proven. A significant
contribution of the biexciton excitation was found to enable two-photon
absorption, making optical excitation process complex. It leads to a dynamic
quantum mechanical interference in the excitation via exciton/biexciton states.
(C) 2000 Elsevier Science B.V. All rights reserved.
66. H.
Kamada, T. Takagahara, H. Ando, J. Temmyo, and T. Tamamura
"Optically
self-induced transparency of exciton excitation in a single semiconductor
quantum dot"
Phys.
Status Solidi A-Appl. Res. 178 (1), 291-296 (2000).
ABSTRACT: The
observation of quantum mechanical interference in the exciton photoluminescence
excitation (PLE) process in a semiconductor quantum dot is reported. A simple
PLE spectroscopy revealed in a single InGaAs quantum dot a dynamic and
continuous evolution of a resonance profile from a peak into a dip and to near
transparency caused by an increase of excitation power density of only a few
100 W/cm(2) A one-photon process via exciton states and a two-photon process
via biexciton states, both of which return to the radiative exciton stale,
interfere quantum mechanically, resulting in a progressive decrease in exciton
absorption under increasing excitation.
67. K.
Kanisawa, H. Yamaguchi, and Y. Hirayama
"Two-dimensional
growth of InSb thin films on GaAs(111)A substrates"
Appl.
Phys. Lett. 76 (5), 589-591 (2000).
ABSTRACT:
Heteroepitaxy of high-quality InSb films was performed directly on GaAs
surfaces by using molecular beam epitaxy. Despite the 14.6% lattice mismatch,
two-dimensionally grown InSb on GaAs(111)A substrates were obtained from the
initial stage, but not on (001) substrates. A conductive layer was formed from
the early stage of the growth on the (111)A surface, and the mobilities and
carrier concentrations of InSb on (111)A substrates suggested a low defect
density due to confinement of the dislocations to the interface. (C) 2000
American Institute of Physics. [S0003-6951(00)03505-1].
68. S. Karimoto
and M. Naito
"New
superconducting lead cuprates prepared by molecular beam epitaxy"
Physica
C 338 (1-2), 92-95 (2000).
ABSTRACT: We
report the synthesis of a new superconducting cuprate PbSr2CuO5+delta (Pb-1201;
T-c similar to 40 K) with a pure PbO charge reservoir layer by a
tow-temperature technique using molecular beam epitaxy (MBE). This new
superconductor is the first member of the Pb-12(n - 1)n homologous series.
Low-temperature synthesis by MBE and an appropriate choice of substrates were essential
to our discovery of Pb-1201 superconductor. This work demonstrates that MBE
provides a novel synthetic route for new cuprates. (C) 2000 Elsevier Science
B.V. All rights reserved.
69. S.
Karimoto and M. Naito
"New
superconducting PbSr2CuO5+delta prepared by a novel low-temperature synthetic
route using molecular beam epitaxy"
Physica
B 284, 1113-1114 (2000).
ABSTRACT: We
report the synthesis of a new superconducting cuprate PbSr2CuO5 + delta (T-c
similar to 40 K) by a novel low-temperature synthetic route using molecular
beam epitaxy. The new superconductor is the first member of the Pb-12(n - 1)n
homologous series. Low-temperature synthesis by MBE and an appropriate choice
of lattice-matched substrates are essential to our discovery of PbSr2CuO5 +
delta superconductor. This work demonstrates that MBE opens up a novel
synthetic route for new cuprates. (C) 2000 Elsevier Science B.V. All rights
reserved.
70. M.
Kasahara, H. Okamoto, K. Takeda, and K. Shiraishi
"Theoretical
study on the electronic and molecular structures of peptide nanotubes"
Abstr.
Pap. Am. Chem. Soc. 219, U144-U144 (2000).
ABSTRACT:
71. M.
Kasahara, H. Okamoto, K. Takeda, and K. Shiraishi
"Theoretical
study on the electronic and molecular structres of peptide nanotubes"
Biochemistry 39
(6), 1568-1568 (2000).
ABSTRACT:
72. N.
Kasai, Y. Jimbo, O. Niwa, T. Matsue, and K. Torimitsu
"Multichannel
glutamate monitoring by electrode array electrochemically immobilized with
enzymes"
Electrochemistry 68
(11), 886-889 (2000).
ABSTRACT: We
developed a novel method for the fabrication of a multichannel glutamate sensor
based on a planar electrode array. By scanning and holding the electrode
potential in a solution containing glutamate oxidase and a polymer to which
horseradish peroxidase and electron-transfer mediator were bound, we
successfully immobilized these enzymes and a mediator on the electrodes of the
electrode array through electrochemical deposition of the polymer. We confirmed
the resulting sensor possessed high sensitivity and selectivity to glutamate.
This multichannel sensor may be useful for the non-invasive, real-time
monitoring of the glutamate distribution in biological samples.
73. N.
Kasai, I. Sugimoto, and M. Nakamura
"Discrimination
of odorants of definite concentrations by using plasma-organic-film-coated QCR
sensors"
Sens.
Actuator B-Chem. 65 (1-3), 114-119 (2000).
ABSTRACT:
Odorant-discrimination experiments were conducted for the major single-odor
substances in various types of botanical species such as fruits and flowers by
using a gas-sensing system consisting of a sensor array of quartz crystal
resonators (QCRs) and a pattern-recognition technique. The sensing devices were
fabricated by radio-frequency sputtering of biomaterials or polymers on to the
QCRs. The 22 tested odorants of definite concentration, 0.1-64 ppm, were well
discriminated by principal component analysis, using the sensors steady-state
and dynamic properties as parameters. From the 1-nearest-neighbor method,
introduced to evaluate the discrimination capability, the best discrimination
was obtained, using the frequency changes in QCRs for longer than 10 min and
the time constant of adsorption at 5 min as parameters, with the success rate
of 83%. This system is thus highly reliable for discriminating trace amounts of
odorants. (C) 2000 Elsevier Science B.V. All rights reserved.
74. S.
Kasapi, S. Lathi, and Y. Yamamoto
"Sub-shot-noise
frequency-modulation spectroscopy by use of amplitude-squeezed light from
semiconductor losers"
J.
Opt. Soc. Am. B-Opt. Phys. 17 (2), 275-279 (2000).
ABSTRACT: We
have demonstrated sub-shot-noise FM spectroscopy on thermal cesium atoms, using
amplitude-squeezed light from a semiconductor laser. The light source used in
our experiment was a custom-made GaAs transverse junction stripe semiconductor
laser featuring broadband amplitude squeezing and a large FM bandwidth. We have
also developed a new technique by which a semiconductor laser can be frequency
modulated with infinitesimally small residual AM and with complete preservation
of the squeezed-amplitude fluctuations. (C) 2000 Optical Society of America
[S0740-3224(00)00802-X].
75. M. Kasu
and N. Kobayashi
"Large
electron field emission from high-quality heavily Si-doped AlN grown by
MOVPE"
J.
Cryst. Growth 221, 739-742 (2000).
ABSTRACT:
Electron field emission (FE) from high-quality AIN grown by metalorganic
vapor-phase epitaxy is studied. The full-widths at half-maximum of the X-ray
rocking curve of undoped and heavily Si-doped (Si density: 2.5 x 10(20) cm(-3))
high-quality AIN were as low as 91 and 94 arcsec, respectively. The heavily
Si-doped AlN showed a maximum FE current of 347 muA and its density was 11
mA/cm(2) Field emission enhancement as a result of Si doping can be explained
by hopping conduction through a Si impurity level. White, red, green, blue
light emission (luminance: about 1200 cd/m(2)) from phosphors excited by the
field-emitted electrons was observed. (C) 2000 Elsevier Science B.V. All rights
reserved.
76. M. Kasu
and N. Kobayashi
"Large
and stable field-emission current from heavily Si-doped AlN grown by
metalorganic vapor phase epitaxy"
Appl.
Phys. Lett. 76 (20), 2910-2912 (2000).
ABSTRACT: We
report on the electron field emission (FE) from heavily Si-doped AlN grown by
metalorganic vapor phase epitaxy. We found that, as the Si-dopant density
increases, the threshold electric field decreases and, consequently, the FE
current from AlN increases drastically. We show that heavily Si-doped
(2.5x10(20) cm(-3)) AlN has a threshold electric field of 34 V/mu m, a maximum
FE current density of 4.8 mA/cm(2), and stable FE current (fluctuation: 3%).
(C) 2000 American Institute of Physics. [S0003-6951(00)03020-5].
77. H. T.
Kato, M. Iwai, Y. Muramatsu, K. Kinoshita, and S. Yoda
"Single
crystal growth of compositionally graded InxGa1-xAs"
Mater.
Sci. Eng. B-Solid State Mater. Adv. Technol. 75
(2-3), 143-148 (2000).
ABSTRACT:
Directional solidifications were carried out by vertical Bridgman method with
GaAs seed and In0.3Ga0.7As feed. Experimental results show that seeding was mon
successful in the case of low temperature gradient than a steep one. Lattice
mismatch of the seed and the grown crystal is small. Single crystals were
reproducibly obtained at low temperature gradient and at small lattice mismatch
in these experiments. The grown single crystal is longer than 20 mm with a
diameter of 14.5 mm. Indium concentration along the growth axis increased as
crystal growth proceeded, which agrees with a compositional profile modeled
from the InAs-GaAs pseudo-binary phase diagram. Electron mobility of initial
grown crystals obtained at lower temperature gradient is higher than that of
crystals grown at higher temperature gradient. (C) 2000 Elsevier Science S.A.
All rights reserved.
78. A.
Kawaharazuka, T. Saku, Y. Hirayama, and Y. Horikoshi
"Formation
of a two-dimensional electron gas in an inverted undoped heterostructure with a
shallow channel depth"
J.
Appl. Phys. 87 (2), 952-954 (2000).
ABSTRACT: We
investigated the dependence of transport characteristics of a two-dimensional electron
gas (2DEG) on channel depth in an inverted undoped GaAs/AlGaAs heterostructure.
We succeeded in forming a high-mobility 2DEG in a sample with 70 nm channel
depth. We controlled the carrier density by varying the back-gate bias over a
wide range. The highest mobility reached 2.3x10(6) cm(2)/Vs at 3.4x10(11)
cm(-2). The relation between mobility and carrier density is determined: the
mobility decreases in a low-carrier-density region as the channel depth
decreases. This result suggests that the scattering due to the remote surface
charges plays a more significant role. (C) 2000 American Institute of Physics.
[S0021-8979(00)02002-8].
79. A.
Kawaharazuka, T. Saku, Y. Horikoshi, and Y. Hirayama
"Channel
depth dependent transport characteristics of a two-dimensional electron gas in
an undoped GaAs/AlGaAs heterostructure"
in
Compound Semiconductors 1999, Institute Of Physics Conference Series
Vol. 166 (Iop Publishing Ltd, Bristol, 2000), pp. 151-154.
ABSTRACT: We
investigated the channel depth dependence of transport characteristics of a
two-dimensional electron gas (2DEG) in an inverted undoped GaAs/AlGaAs
heterostructure. We succeeded in forming a 2DEG with high mobility in a sample
having a channel depth of 70 nm. The relation between mobility and carrier
density is determined: the mobility decreases in a low-carrier-density region
as the channel depth decreases. This result suggests that the scattering due to
the remote surface charges plays a more significant role.
80. T.
Kawamura, Y. Watanabe, Y. Utsumi, K. Uwai, J. Matsui, Y. Kagoshima, Y. Tsusaka,
and S. Fujikawa
"In
situ observation of superstructures on InP(001) surface under hydrogen
atmospheric environment with using grazing incidence X-ray diffraction"
J.
Cryst. Growth 221, 106-110 (2000).
ABSTRACT:
Because of the difficulties of using electron-based techniques in the
metalorganic vapor-phase epitaxy (MOVPE) environment, an in situ X-ray
diffractometer that combines a goniometer and reactor chamber was developed.
Consequent measurements of P-rich InP(001) surface grown by MOVPE show the
surface has a (2 x 1) structure. Calculations based on a P-dimer model suggest
that this structure is composed of P-dimers whose bonding is parallel to the
[(1) over bar 10] direction and indicates indium displacement in the second
layer. (C) 2000 Elsevier Science B.V. All rights reserved.
81. T.
Kawamura, Y. Watanabe, Y. Utsumi, K. Uwai, J. Matsui, Y. Kagoshima, Y. Tsusaka,
and S. Fujikawa
"Reconstruction
of an InP(001) surface grown by metalorganic vapor phase epitaxy in atmospheric
hydrogen environment"
Appl.
Phys. Lett. 77 (7), 996-998 (2000).
ABSTRACT: A
reconstructed surface of InP (001) substrate, grown by metalorganic vapor phase
epitaxy under atmospheric hydrogen environment, is investigated by using
grazing incident x-ray diffraction. Fractional-order diffractions of (n/2 m)
were observed, showing the existence of a (2 x 1) domain on the surface.
Calculations based on the P-dimer model suggest that there are P dimers whose
bonding is parallel to the [(1) over bar 10] direction and indium displacement
in the second layer. (C) 2000 American Institute of Physics.
[S0003-6951(00)02733-9].
82. K.
Kinoshita, H. Kato, S. Matsumoto, and S. Yoda
"Growth
of homogeneous In1-xGaxSb crystals by the graded solute concentration
method"
J.
Cryst. Growth 216 (1-4), 37-43 (2000).
ABSTRACT: We
propose a new crystal growth method named "the graded solute concentration
method" for obtaining homogeneous mixed crystals from their melts in the
presence of residual acceleration of the order of 10(-3)-10(-4) G in
microgravity. In this method, the feed with preinstalled solute concentration
profile is used for compensating solute loss at the solid-liquid (S/L) interface
due to convection caused by the residual acceleration. By the preliminary
ground-based experiments using capillary tubes with a 1.5 mm bore, we obtained
homogeneous In0.4Ga0.6Sb and In0.2Ga0.8Sb crystals. These results show the
validity of the proposed method. (C) 2000 Elsevier Science B.V. All rights
reserved.
83. T.
Kiyokura, F. Maeda, Y. Watanabe, Y. Iketaki, K. Nagai, Y. Horikawa, M. Oshima,
E. Shigemasa, and A. Yagishita
"Throughput
measurement of a multilayer-coated Schwarzschild objective using synchrotron
radiation"
Opt.
Rev. 7 (6), 576-578 (2000).
ABSTRACT: The
throughput of a Schwarzschild objective using undulator synchrotron radiation
was measured. Conventionally, the throughput was estimated from the squared
reflectivity of one multilayer mirror and from the obstruction ratio. However,
we evaluated the transmission ratio from the input and output photon flux using
a precisely calibrated monochromatic beam from an undulator light source. It
was found that the objective has a maximum throughput of 8.5% at a wavelength
of 13.9 nm.
84. G.
Klimovitch, F. Tassone, Y. Yamamoto, and H. Cao
"Stimulated
resonant tunneling into quantum well excitons"
Phys.
Lett. A 267 (4), 281-286 (2000).
ABSTRACT:
Stimulated electron resonant tunneling into exciton states is investigated
within the pairing approximation and the interacting boson approximation. The
tunneling current saturates at large densities due to the fermionic nature of
exciton constituents. Conditions under which stimulated tunneling can be
observed experimentally are described. (C) 2000 Published by Elsevier Science
B.V. All rights reserved.
85. M.
Koashi and M. Ueda
"Exact
eigenstates and magnetic response of spin-1 and spin-2 Bose-Einstein
condensates"
Phys.
Rev. Lett. 84 (6), 1066-1069 (2000).
ABSTRACT: The
exact eigenspectra and eigenstates of spin-1 and spin-2 Bose-Einstein
condensates (BECs) are found, and their response to a weak magnetic field is
studied and compared with their mean-field counterparts. Whereas mean-field
theory predicts the vanishing population of the zero magnetic-quantum-number
component of a spin-1 antiferromagnetic BEG, the component is found to become
populated as the magnetic field decreases. The spin-2 BEC exhibits an even
richer magnetic response due to quantum correlations among three bosons.
86. N.
Kobayashi and Y. Kobayashi
"In-situ
optical monitoring of surface morphology and stoichiometry during GaN metal
organic vapor phase epitaxy"
Appl.
Surf. Sci. 159, 398-404 (2000).
ABSTRACT: The
surfaces during GaN metalorganic vapor phase epitaxy (MOVPE) were in-situ monitored
by shallow-angle reflectance using ultraviolet (uv) light and were compared
between the growths on sapphire and on 6H-SiC substrates. By this method,
stable monitoring is possible without an influence of strong and visible
black-body radiation from the substrate heated to high temperatures. The
growth-rate was successfully monitored by optical interference, and the
morphological change was detected by the reflectivity change due to Rayleigh
scattering. The surface of AIN buffer layer deposited on the (0001) sapphire
substrate roughens at the thickness thinner than 30 nm, when the temperature is
raised to the growth temperature of GaN. From the period of interference
oscillation observed, the growth-rate on the (0001) SiC substrate is almost
constant but, on the sapphire substrate, the growth-rate is about 14%
decelerated in the thickness range approximately from 70 to 140 nm due to the
coalescence of islands by lateral growth. Surface photoabsorption (SPA) was
applied to monitor the chemical stoichiometry of GaN surface during growth. It
is found that the uniform growth dominated by step-now mode is achieved by
Ga-rich stoichiometry in H-2 carrier gas. The surface process during uniform
growth of GaN is also proposed. (C) 2000 Elsevier Science B.V. All rights
reserved. PACS: 81.05.Ea, 81.15.Gh; 82.30.Lp.
87. S.
Kodama, Y. Furumura, K. Kinoshita, H. Kato, and S. Yoda
"Single
crystalline bulk growth of In0.3Ga0.7As on GaAs seed using the multi-component
zone melting method"
J.
Cryst. Growth 208 (1-4), 165-170 (2000).
ABSTRACT: A
28 mm in length and 15 mm in diameter single-crystalline InxGa1-xAs ternary
bulk crystal was grown on GaAs seed crystal using the multi-component zone
melting method. The InAs composition of the grown crystal was gradually
increased from 0.04 at the initial growth interface to 0.33 by decreasing the
growth temperature as in the vertical gradient freeze method during growth of
24 mm length, and then maintained at 0.34 +/- 0.01 for the following growth of
4 mm length by making the sample travel at a rate nearly equal to the growth
rate without lowering the furnace temperature. This combination of temperature
and sample traveling rate control enabled the growth of homogeneous
In0.3Ga0.7As ternary bulk crystal. (C) 2000 Elsevier Science B.V. All rights
reserved.
88. J. R.
Koe, M. Fujiki, M. Motonaga, and H. Nakashima
"Temperature-dependent
helix-helix transition of an optically active poly(diarylsilylene)"
Chem.
Commun. (5), 389-390 (2000).
ABSTRACT: The
poly(diarylsilylene) copolymer mainchain helix in (Ar*Si-2)(x)(Ar2Si)(1-x) [Ar*
= 3-(S)-2-methylbutylphenyl, Ar = 4-butylphenyl, x = 0.2] undergoes a thermally
driven inversion of helical screw sense with a transition temperature of -10
degrees C.
89. J. R.
Koe, M. Fujiki, H. Nakashima, and M. Motonaga
"Helical
diarylpolysilanes: Effects of higher-order structure on optical activity"
Abstr.
Pap. Am. Chem. Soc. 219, U447-U447 (2000).
ABSTRACT:
90. T. Koga,
S. B. Cronin, M. S. Dresselhaus, J. L. Liu, and K. L. Wang
"Experimental
proof-of-principle investigation of enhanced Z(3D)T in (001) oriented Si/Ge
superlattices"
Appl.
Phys. Lett. 77 (10), 1490-1492 (2000).
ABSTRACT: An
experimental proof-of-principle of an enhanced Z(3D)T (thermoelectric figure of
merit) is demonstrated using (001) oriented Si/Ge superlattices. The highest
value of the experimental Z(3D)T at 300 K for a (001) oriented Si(20
Angstrom)/Ge(20 Angstrom) superlattice is 0.1 using kappa = 5 Wm(-1) K-1, for
the in-plane thermal conductivity, which is a factor of seven enhancement
relative to the estimated value of Z(3D)T = 0.014 for bulk Si. The good
agreement between experiment and theory validates our modeling approach
(denoted as "carrier pocket engineering") to design superlattices
with enhanced values of Z(3D)T. Proposals are made to enhance the experimental
values of Z(3D)T for Si/Ge superlattices even further. (C) 2000 American
Institute of Physics. [S0003-6951(00)05136-6].
91. T. Koga,
O. Rabin, and M. S. Dresselhaus
"Thermoelectric
figure of merit of Bi/Pb1-xEuxTe superlattices"
Phys.
Rev. B 62 (24), 16703-16706 (2000).
ABSTRACT: An
enhanced thermoelectric figure of merit Z(3D)T is predicted for
Bi/(111)Pb1-xEuxTe superlattices. The values of Z(3D)T obtained for x
approximate to1 superlattices are 2.31, 1.55, and 1.61 at 300, 150, and 77 K,
respectively, showing that they are promising candidates for thermoelectric
elements in the temperature range 77-300 K. Even with x as small as 0.1, where
the conduction-band offset DeltaE(c) is estimated to be 0.25 eV, the predicted
Z(3D)T values are 1.75, 1.16, and 1.18 at 300, 150, and 77 K, respectively. It
is proposed that other families of Bi-based superlattices, such as Bi/(111)CdTe
superlattices, should also be good candidates for low-temperature
thermoelectric elements.
92. H. Kudo,
N. Nakamura, K. Shibuya, K. Narumi, S. Yamamoto, H. Naramoto, K. Sumitomo, and
S. Seki
"Ion-induced
electron emission from Si crystal targets covered with noncrystalline Si
layers"
Nucl.
Instrum. Methods Phys. Res. Sect. B-Beam Interact. Mater. Atoms 168
(2), 181-191 (2000).
ABSTRACT:
Ion-induced electron emission has been studied for Si crystal targets bombarded
by similar to 100 keV/u H+, He+, and 3.5 MeV/u O8+. Under channeling incidence
conditions, we have measured the dependence of the continuum electron yield on
the thickness of an overlaid noncrystalline Si layer which increases the number
of unshadowed atoms near the crystal surface. The electron yields in the
channeling and nonchanneling cases are successfully accounted for using the two
parameters determined from the experiments, i.e., the effective target
thickness associated with the high-energy shadowing effect mainly on Si
L-shells and the effective escape length for the electron yield. (C) 2000
Elsevier Science B.V. All rights reserved.
93. H. Kudo,
S. Seki, K. Sumitomo, K. Narumi, S. Yamamoto, and H. Naramoto
"Ion-induced
electron measurements using crystal targets overlaid with noncrystalline
layers"
Nucl.
Instrum. Methods Phys. Res. Sect. B-Beam Interact. Mater. Atoms 164,
897-902 (2000).
ABSTRACT: We
have measured continuum electron yields from Si crystals covered with
noncrystalline Si layers of 150-350 Angstrom thicknesses using 8.0 MeV/u H+ and
He2+. These layers provide unshadowed subsurfaces from which target electrons
are recoiled under channeling incidence conditions. The production and escape
processes of the electrons can be well understood using a few quantities
determined from these experiments. The present experimental approach allows
general understanding of the continuum electron spectra from solid targets. (C)
2000 Elsevier Science B.V. All fights reserved.
94. N.
Kumada, A. Sawada, Z. F. Ezawa, S. Nagahama, H. Azuhata, K. Muraki, T. Saku,
and Y. Hirayama
"Doubly
enhanced skyrmions in nu=2 bilayer quantum Hall states"
J.
Phys. Soc. Jpn. 69 (10), 3178-3181 (2000).
ABSTRACT:
Skyrmion excitations were measured and compared for the first time in the
bilayer quantum Hall (QH) state at the Landau-level filling factor nu = 2 and
in the monolayer QH state at nu = 1. The observed number of flipped spins,
N-spin, is 14 in the bilayer sample with a large tunnelling gap, and N-spin = 7
in the bilayer sample with a small tunnelling gap, while it is N-spin = 7 in
the monolayer sample. The difference is interpreted to be due to the interlayer
exchange interaction.
95. K.
Kumakura, T. Makimoto, and N. Kobayashi
"High
hole concentrations in Mg-doped InGaN grown by MOVPE"
J.
Cryst. Growth 221, 267-270 (2000).
ABSTRACT: We
investigated the electrical properties of Me-doped InxGa1-xN (0 less than or
equal to x < 0.75) grown by metalorganic vapor-phase epitaxy with various
growth conditions, such as Mg-doping concentration, growth-rate and growth
temperature. The hole concentration depends on the growth-rate, the In mole
fraction and the crystal quality of the InGaN layers. The hole concentration of
Mg-doped InxGa1-xN layers below x = 0.15 increased with the In mole fraction,
while those above x = 0.15 decreased. We realized the p-type InGaN with the
room-temperature hole concentration above 10(18)cm(-3) and obtained the maximum
hole concentration of 7.8 x 10(18) cm (-3) for x = 0.2 by optimizing the growth
conditions. (C) 2000 Elsevier Science B.V. All rights reserved.
96. K.
Kumakura, T. Makimoto, and N. Kobayashi
"Activation
energy and electrical activity of Mg in Mg-doped InxGa1-xN (x < 0.2)"
Jpn.
J. Appl. Phys. Part 2 - Lett. 39 (4B), L337-L339 (2000).
ABSTRACT: We
investigated the electrical properties of Mg-doped InGaN with an In mole
fraction of less than 0.2 grown by metaloganic vapor phase epitaxy. We obtained
p-type InGaN with a hole concentration above 10(18) cm(-3) at room temperature.
The hole concentrations of Mg-doped In0.04Ga0.96N and In0.14Ga0.86N were 1.2 x
10(18) and 6.7 x 10(18) cm-3, respectively, while that of Mg-doped GaN was 3.0
x 10(17) cm(-3) with the same Mg doping concentration. The activation energy of
Mg in InGaN, calculated from the temperature dependence of the hole
concentration, decreases with the increase in the In mole fraction.
Furthermore, the electrical activity of Mg in InGaN increases with the In mole
fraction. As a result, higher hole concentrations were obtained at room
temperature for Mg-doped InxGa1-xN (x < 0.2) with higher In mole fractions.
97. K.
Kumakura, T. Makimoto, and N. Kobayashi
"Enhanced
hole generation in Mg-doped AlGaN/GaN superlattices due to piezoelectric
field"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 39
(4B), 2428-2430 (2000).
ABSTRACT: We
investigated the electrical properties of uniformly Mg-doped AlGaN/GaN
superlattices (SLs) with various Al mole fractions and SL period thicknesses.
We found that their sheet hole concentration depended strongly on the Al mole
fraction and SL period thickness. We found the maximum spatial averaged hole
concentrations for SLs with period thicknesses of 360 Angstrom and 100 Angstrom
to be 3 x 10(18) cm(-3) at room temperature. The resistivities of the SLs were
less temperature dependent than those of GaN and AlGaN, indicating that the
enhanced hole generation in these SLs could be ascribed to the large energy
shift of the valence band edge due to the piezoelectric field.
98. K.
Kumakura, T. Makimoto, and N. Kobayashi
"Efficient
hole generation above 10(19) cm(-3) in Mg-doped InGaN/GaN superlattices at room
temperature"
Jpn.
J. Appl. Phys. Part 2 - Lett. 39 (3AB), L195-L196 (2000).
ABSTRACT: We
achieved spatially averaged hole concentrations above 10(19) cm(-3) at room
temperature in Mg-doped InxGa1-xN/GaN (4nm/4nm) superlattices grown by
metalorganic vapor phase epitaxy. The hole concentrations for the InxGa1-xN
/GaN superlattices increased with the In mole fraction, and the maximum hole
concentration reached 2.8 x 10(19) cm-3 for the In0.22Ga0.78N/GaN superlattice.
The hole concentrations for the superlattices are larger than those for the
InGaN bulk layers with the same average In mole fraction. The weak temperature
dependence of the resistivities for InGaN/GaN superlattices with higher In mole
fractions indicates highly efficient hole generation in the superlattice.
99. E.
Kuramochi, M. Notomi, T. Tamamura, T. Kawashima, S. Kawakami, J. Takahashi, and
C. Takahashi
"Drilled
alternating-layer structure for three-dimensional photonic crystals with a full
band gap"
J.
Vac. Sci. Technol. B 18 (6), 3510-3513 (2000).
ABSTRACT: A
new three-dimensional photonic crystal structure is designed to simplify
fabrication. A calculation of the band structure predicts that this photonic
crystal has a complete photonic band gap in all directions. The entire
three-dimensional periodic structure, except for the vertically drilled holes,
is formed by automatic shaping during bias sputtering deposition. The
fabrication technologies used to construct this photonic crystal are electron
beam lithography, bias sputtering, and fluoride aas electron cyclotron
resonance etching. Our preliminary fabrication reveals that each technology can
be controlled well enough to lead to the creation of a photonic band gap
material for an optical communication wavelength. (C) 2000 American Vacuum
Society. [S0734-211X(00)07806-9].
100. T. D. Ladd, J. R. Goldman,
F. Yamaguchi, and Y. Yamamoto
"Decoherence
in crystal lattice quantum computation"
Appl.
Phys. A-Mater. Sci. Process. 71 (1), 27-36 (2000).
ABSTRACT:
Nuclear magnetic resonance (NMR) quantum computation in a crystal lattice holds
more promise for scalability than its solution NMR counterpart, but dephasing
is a severe concern. Pulse sequence refocusing can help bring the qubit
dephasing time closer to the limit of the intrinsic decoherence time, but the
intrinsic transverse relaxation time (T-2) and the longitudinal relaxation time
(T-1) of the crystal must be sufficiently long for a successful implementation.
We discuss these time scales and their relation to parameters relevant to
quantum computation for several crystal types, discussing in detail the
examples of CaF2, MnF2. and CeP. Included in the calculation of coherence times
for CeP is the development of spin-wave spectra in a type-1 antiferromagnetic
FCC lattice. PACS: 03.67.Lx; 76.60.Es; 75.30.Ds.
101. D. W. Leung, I. L. Chuang,
F. Yamaguchi, and Y. Yamamoto
"Efficient
implementation of coupled logic gates for quantum computation"
Phys.
Rev. A 6104 (4), art. no.-042310 (2000).
ABSTRACT:
Most natural Hamiltonians do not couple specific pairs of quantum bits and
spurious couplings occur along with the intended one. We present an efficient
scheme that couples any designated pair of spins in heteronuclear spin systems.
The scheme is based on the existence of Hadamard matrices. For a system of n
spins with pairwise coupling, the scheme concatenates cn intervals of system
evolution and uses at most cn(2) pulses where c approximate to 1. Our results
demonstrate that, in many systems, selective recoupling is possible with linear
overhead, contrary to common speculation that exponential effort is always
required.
102. T. Machida, S. Ishizuka,
K. Muraki, Y. Hirayama, and S. Komiyama
"Resistance
fluctuations in integer quantum-Hall transitions"
Physica
E 6 (1-4), 152-155 (2000).
ABSTRACT: We
have studied the resistance fluctuations (RF) in integer quantum-Hall
transitions for high-mobility two-dimensional electron gas systems. The role of
coherence in RF is examined by investigating the conductance through two
scattering regions, that are spatially separated but interfere
quantum-mechanically with each other. The phase coherence does not play a
substantial role in determining the pattern of RF, whereas it affects the
amplitude of RF. (C) 2000 Elsevier Science B.V. All rights reserved.
103. F. Maeda, M. Sugiyama, and
Y. Watanabe
"GaSb(001)
4 x 2-In surface structure studied by core-level photoelectron spectroscopy and
X-ray standing-wave analysis"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 39
(7B), 4351-4354 (2000).
ABSTRACT: The
surface structure of GaSb(001) 4 x 2-In was investigated by core-level
photoelectron spectroscopy (CLPES) using synchrotron radiation and X-ray
standing-wave (XSW) analysis. From the CLPES measurement, we found that the 4 x
2 surface was mainly composed of single chemical bondings, which could be
assigned to In-Sb bonding. This indicated that an In-Sb molecular layer
terminated this 4 x 2 surface. In addition, the In atom position was analyzed
by XSW using two different asymmetric (111) and (1-11) reflections. The
coherent position values of 0.684 for (111) and 0.015 for (1-11) that were
obtained indicated that the In atom position was higher than the top Sb atom
position of Sb-double-layer. From these results, we propose a surface local
bonding model for GaSb(001) 4 x 2-In, in which the Sb-double layer remains and
In atoms terminate the surface.
104. F. Maeda, M. Sugiyama, and
Y. Watanabe
"In-induced
surface reconstruction on GaSb(001)"
Phys.
Rev. B 62 (3), 1615-1618 (2000).
ABSTRACT:
In-induced surface reconstructions on GaSb(001), prepared by molecular-beam
epitaxy, have been investigated in situ by reflection high-energy electron
diffraction and core-level photoelectron spectroscopy. Although In grew three
dimensionally at room temperature, a 1x3 reconstructed surface appeared at 430
degrees C after the substrates were annealed. After this 1x3 surface was
obtained, 4x3 and/or 4x2 reconstructions were observed as the substrate was
cooled, which induced an increase in the In coverage in the two-dimensional
(2D) layer. On the 4x2 surface, we found the saturation of the Tn coverage in
the 2D layer and a single bonding state of In-Sb, while several bonding states
were observed on the 1x3 surface. This indicates that a drastic atomic
rearrangement results in the termination with an InSb molecular layer at the
1x2 surface.
105. F. Maeda and Y. Watanabe
"Real-time
analysis of alternating growth on GaAs(001) by core-level photoelectron
spectroscopy"
Appl.
Surf. Sci. 162, 319-325 (2000).
ABSTRACT: The
alternating growth of GaAs on a (001) surface was analyzed by time-resolved
core-level photoelectron spectroscopy (CLPES) and measuring reflection
high-energy electron diffraction (RHEED) specular beam intensity. When looking
at a Ga supply period, a saturation of Ga coverage was found from the
time-dependence of Ga CLPES intensity. The RHEED specular beam intensity
decreased even after the saturation coverage of Ga. These results indicate that
Ga droplets begin to grow after Ga has been grown laterally. The inflection
points of photoelectron intensity change were found at about half a monolayer
of Ga supply at a substrate temperature of 560 degrees C. The spectrum analysis
of the time-resolved CLPES clarifies that the Ga adsorption site changes at
about half a monolayer of Ga supply. These results show the potential of using
time-resolved CLPES for the real-time analysis of the growth process. (C) 2000
Elsevier Science B.V. All rights reserved.
106. N. Maeda, T. Saitoh, K.
Tsubaki, T. Nishida, and N. Kobayashi
"Two-dimensional
electron gas transport properties in AlGaN/(In)GaN/AlGaN double-heterostructure
field effect transistors"
Mrs.
Internet J. Nitride Semicond. Res. 5, art. no.-W4.7 (2000).
ABSTRACT:
Two-dimensional electron gas transport properties have been investigated in
nitride double-heterostructures. A striking effect has been observed that the two-dimensional
electron gas mobility has been drastically enhanced in the AlGaN/GaN/AlGaN
double-heterostructure, compared with that in the conventional AlGaN/GaN
single-heterostructure. The observed mobility enhancement has been shown to be
mainly due to the enhanced polarization-induced electron confinement in the
double-heterostructure, and additionally due to the improvement of the
interface roughness in the structure. Device operation of an AlGaN/GaN/AlGaN
double-heterostructure field effect transistor has been demonstrated: a maximum
transconductance of 180 mS/mm has been obtained for a 0.4 mum-gate-length
device. In the double-heterostructure using InGaN channel, the increased
capacity for the two-dimensional electron gas has been observed. The AlGaN/(In)GaN/AlGaN
double-heterostructures are effective for improving the electron transport
properties.
107. N. Maeda, T. Saitoh, K.
Tsubaki, T. Nishida, and N. Kobayashi
"Enhanced
effect of polarization on electron transport properties in AlGaN/GaN double-heterostructure
field-effect transistors"
Appl.
Phys. Lett. 76 (21), 3118-3120 (2000).
ABSTRACT: In
order to understand the effect of polarization on the electron transport
properties in AlGaN/GaN heterostructures, the dependence of the two-dimensional
electron gas mobility on the density has been examined both in the GaN single-
and 200-Angstrom GaN double- heterostructure field-effect transistors, by means
of the Hall effect measurement under the gate-voltage application at 4.2 K. In
the single heterostructure, a maximum mobility of 5700 cm(2)/V s has been
obtained at 9.0x10(12) cm(-2); whereas in the double heterostructure, a higher
maximum mobility of 8100 cm(2)/V s has been obtained at a lower electron
density of 6.8x10(12) cm(-2). The results have been analyzed in terms of
potential profiles and electron distributions in both structures where both
piezoelectric and spontaneous polarization effects are taken into account. The
analysis has shown that the observed mobility enhancement is mainly due to the
enhanced polarization-induced electron confinement in the double
heterostructure and, additionally, to the improvement of the interface
roughness in the structure. (C) 2000 American Institute of Physics.
[S0003-6951(00)01421-2].
108. T. Makimoto, K. Kumakura,
and N. Kobayashi
"Reduced
damage of electron cyclotron resonance etching by In doping into p-GaN"
J.
Cryst. Growth 221, 350-355 (2000).
ABSTRACT: We
investigated the effect of In atoms in p-GaN on the damage induced by electron
cyclotron resonance etching. After etching the surface of p-GaN without In
atoms, the I-V characteristics between two Ni/Au electrodes on the surface
showed non-Ohmic behavior. This is ascribed to the damage induced by this
etching process, as previously reported. The Ohmic characteristics were much
improved for p-GaN doped with In atoms compared with those for p-GaN without In
atoms. The Ohmic characteristics were improved as the In mole fraction in the
p-(In)GaN was increased. The non-Ohmic behavior arises from the damaged layer
between the Ni/Au electrode and the p-(In)GaN layer. This damaged layer is
considered to become thinner as the In mole fraction is increased, resulting in
improved Ohmic characteristics. (C) 2000 Elsevier Science B.V. All rights
reserved.
109. H. Masuda, K. Yasui, T.
Yanagishita, M. Nakao, T. Tamamura, and K. Nishio
"Direct
nanomolding of semiconductor single crystals"
Jpn.
J. Appl. Phys. Part 2 - Lett. 39 (3AB), L256-L258 (2000).
ABSTRACT: An
ordered array of concaves of nanometer-scale dimensions was fabricated by a
direct molding process on an InP single crystal using a SiC master mold. The
obtained array of concaves could be applied for the preparation of an ordered
textured surface of InP by a post-etching treatment. The treatment in
hydrofluoric acid (HF) solution generated a highly ordered and textured surface
composed of uniform pyramidal or triangular pits. The mold could be used
repeatedly, and this method enables simple maskless patterning of semiconductor
single crystals.
110. K. Matsuda, S. Tanda, M.
Shiobara, Y. Okajima, K. Yamaya, and N. Hatakenaka
"Quantum
collective dynamics of charge-density waves in quasi-one-dimensional orthorhombic
TaS3"
J.
Phys. Soc. Jpn. 69 (4), 1251-1252 (2000).
ABSTRACT:
111. K. Matsunaga, M. Nishida,
D. Matsumoto, S. Kurihara, N. Hatakenaka, and H. Takayanagi
"Josephson
phase dynamics in He-3 weak links"
Physica
B 284, 285-286 (2000).
ABSTRACT: We
propose a simple phenomenological model for dissipative dynamics of a
superfluid. Qualitative agreement between the results of our numerical
calculations and of the experiment on a superfluid helium three weak link
system gives strong support for our model. (C) 2000 Elsevier Science B.V. All
rights reserved.
112. T. Matsuoka, T. Ito, and
T. Kaino
"First
plastic optical fibre transmission experiment using 520nm LEDs with intensity
modulation/direct detection"
Electron.
Lett. 36 (22), 1836-1837 (2000).
ABSTRACT: A
plastic optical fibre (POF) transmission experiment utilising green LEDs at a
wavelength of 520nm is reported. The transmission loss of the 100m POF was
10dB, which is considerably lower than the loss for red (660nm) and blue
(470nm) LEDs. The receiver sensitivity at 30Mbit/s was -20.8dB at 10(-9) bit
error rate, which suggests the possibility of a longer length signal
transmission, 200m or longer.
113. M. Mitsunaga, M.
Yamashita, and H. Inoue
"Absorption
imaging of electromagnetically induced transparency in cold sodium atoms"
Phys.
Rev. A 62 (1), art. no.-013817 (2000).
ABSTRACT:
Transmissivity of up to 200% has been observed in an absorption imaging study
of electromagnetically induced transparency in cold sodium atoms, when a
focused coupling beam is applied near the edge of the atom cloud. The signal
behavior strongly depends on the frequency difference between the probe beam
and the coupling beam. Such high transmissivity can be attributed to the strong
focusing effect of the probe beam, when it propagates in a medium with
spatially inhomogeneous refractive index induced by the coupling beam. A
detailed numerical analysis based upon the Maxwell propagation equations is
presented.
114. N. A. Mortensen and G.
Bastian
"Side-gate
modulation of critical current in mesoscopic Josephson junction"
Superlattices
Microstruct. 28 (3), 231-237 (2000).
ABSTRACT: We
study the normal state conductance and the Josephson current in a
superconductor-2DEG-superconductor structure where the size/shape of the
2DEG-region can be modified by an additional side-gate electrode. The
considered transport properties follow from the retarded Green function which
we compute by employing a tight-binding-like representation of the Hamiltonian
in the 2DEG region. Our model studies offer a qualitative demonstration of the
recently observed effects caused by side-gate modulation. (C) 2000 Academic
Press.
115. K. Muraki, N. Kumada, T.
Saku, and Y. Hirayama
"n(+)-GaAs
back-gated double-quantum-well structures with full density control"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 39
(4B), 2444-2447 (2000).
ABSTRACT: We
present the fabrication of a novel double-quantum-well (DQW) structure, in
which the upper electron layer is supplied via modulation doping while the
lower one is fully induced through the field effect from an n(+)-GaAs back
Sate. Low-temperature transport measurements demonstrate that two-dimensional
electron gases with equally high mobilities are successfully formed in the
lower as well as in the upper QWs. By this approach, the electron density in
the lower layer can be controlled over a wide range with a small back-gate
bias, and hence the electron-density distribution in the DQW can be tuned
arbitrarily by using a front gate in conjunction with the back gate.
116. T. Murata, S. Kishimoto,
K. Maezawa, T. Mizutani, T. Ishii, and T. Tamamura
"An
electron wave interference transistor with a novel recess-etched grating
structure fabricated using electron beam lithography"
in
Compound Semiconductors 1999, Institute Of Physics Conference Series
Vol. 166 (Iop Publishing Ltd, Bristol, 2000), pp. 347-350.
ABSTRACT: We
have successfully fabricated electron wave interference transistors (EWITs)
with a novel recess-etched grating structure. Fine patterns with 60-nm period
were fabricated by 100-keV electron beam (EB) lithography with a novel
nanocomposite resist. A clear transconductance (g(m)) oscillation was observed
in g(m)-V-G characteristics of the EWITs at temperatures up to 50 K. It was
confirmed by analyzing the index of g(m) peaks that the observed g(m)
oscillation was due to the electron wave interference caused by the periodic
potential modulation in the channel produced by the recess-etched grating under
the gate. The calculation of the transmission coefficient (TT) of electrons in
the channel of the EWIT shows that it is possible to observe clear interference
phenomena if the number of the grating is larger than 10.
117. M. Nagase and K. Kurihara
"Imaging
of Si nano-patterns embedded in SiO2 using scanning electron microscopy"
Microelectron.
Eng. 53 (1-4), 257-260 (2000).
ABSTRACT:
Detailed shapes of embedded Si nanostructures were clearly observed through a
SiO2 layer using scanning electron microscopy (SEM). We Pound a new imaging
mechanism by which secondary electron (SE) yield from the oxide surface is
greater where an embedded Si structure exists. In the range of acceleration
voltages from 5 to 200 kV, we found that 30 kV provides high contrast and high
resolution. Controlling the surface contrast by depositing a contaminated film
using electron beam irradiation yields a clear, high-resolution SEM image of
sub-10-nm Si structures embedded in a 60-nm-thick oxide. The combination of a
non-destructive observation method based on SEM with a method based on AFM,
which was demonstrated previously, provides detailed information on the
three-dimensional shape of embedded Si nanodevices.
118. M. Naito and M. Hepp
"Superconducting
T '-La2-xCexCuO4 films grown by molecular beam epitaxy"
Jpn.
J. Appl. Phys. Part 2 - Lett. 39 (6A), L485-L487 (2000).
ABSTRACT: In
this letter we report the synthesis of superconducting T'-La2-xCexCuO4 on
SrTiO3(001) by molecular beam epitaxy. Although T'-La2-xCexCuO4 with a very
limited range of x can be prepared by bulk synthesis using rather complicated
techniques, this compound is very easy to obtain by thin film synthesis.
Crucial to our success was the use of SrTiO3 substrates, which seems to
stabilize the formation of the T' structure by an epitaxial effect. The best
T-c was similar to 30 K by onset and similar to 28 K by zero resistance, which
was obtained for x = 0.109. The resistivity showed a metallic temperature
dependence, and the film's overall behavior was similar to that for the best
(Nd, Ce)(2)CuO4 or (Pr, Ce)(2)CuO4 films. Moreover, the single phase of the T'
structure formed for a composition range of 0.09 < x < 0.22, which is
much wider than for previously reported bulk synthesis.
119. M. Naito, H. Yamamoto, and
H. Sato
"Intrinsic
problem of cuprate surface and interface: why good tunnel junctions are
difficult to fabricate"
Physica
C 335 (1-4), 201-206 (2000).
ABSTRACT: In
this article, we point out the key issue to fabricate high-T-c tunnel junctions
on the basis of our recent systematic photoemission studies on MBE grown films.
As a general feature for cuprates, the Cu-O bond is weak. Therefore, the redox
reaction easily occurs at the interface between the cuprate surface and
overlayers. This causes significant oxygen deficiencies, leading to serious
degradation or complete destruction of superconductivity in the interface
region. This is the reason why good tunnel junctions have not been successfully
fabricated on high-ir, superconductors. Furthermore, we warn that all surface
or interface-sensitive experiments, such as tunneling spectroscopy (including
STM), various Josephson-current-based experiments, and even XPS/UPS may suffer
from this problem, and hence may not lead to correct conclusions. (C) 2000
Elsevier Science B.V. All rights reserved.
120. H. Nakano and H.
Takayanagi
"Influence
of phase quantum fluctuations on superconducting proximity correction in
normal-metal wire conductance"
Phys.
Rev. B 61 (22), 15398-15411 (2000).
ABSTRACT: The
influence of the charging effect on the proximity correction in the conductance
of a mesoscopic superconductor(S)/normal-metal(N) coupled system is
theoretically investigated. The most important contribution of the proximity
correction in the conductance of a diffusive normal metal comes from the
correction in the local conductivity delta sigma(r). The correction in the
conductance is given by delta G = (1/L-N(2))integral(vol.)delta sigma(r)dr.
Because of the retro property of Andreev reflection and the long rangeness of
the Cooperon (particle-particle ladder), Andreev reflection at the SIN
interface affects the local conductivity at a point in the normal region far
from the interface (within the phase coherence length L-phi) If the SIN
interface is very small and has a low transparency, single Andreev reflection
is strongly suppressed by the Coulomb blockade at a low temperature
(k(B)T<E-C, E-C = e(2)/2C) in an exponential manner exp{-4E(C)/(k(B)T)},
where C is the capacitance of the SIN junction. Nevertheless, the proximity
correction in the conductance is only suppressed with power law k(B)T/(4E(C))
because the charged state is an intermediate state in the process of the
proximity correction in the conductivity. This is quite different from the
charging effect on the proximity correction of the current flowing through the
SIN interface, which is strongly suppressed by the charging effect.
121. H. Nakano and H.
Takayanagi
"Superconducting
proximity effect and charging effect on the normal transport in normal-metal
(semiconductor) wire"
J.
Low Temp. Phys. 118 (5-6), 653-662 (2000).
ABSTRACT: We
theoretically investigated superconducting proximity corrections of the
conductance of a mesoscopic metal wire in terms of the Kubo-formula. In
diagrammatic expression, the electromagnetic response kernel is quite similar
to that of reproducible conductance fluctuation However, the proximity
correction modifies the average conductance of the wire even though the latter
gives a mesoscopic fluctuation. This Kubo-formula expression is applicable to
the analysis of charging effects on the proximity correction in a
superconductor(S)/Mesoscopic-normal-metal-wire(N) hybrid system with a very
small S/N interface. Although the charging effect exponentially suppresses Andreev
reflections at the S/N interface, the proximity correction survives. We propose
an experiment to confirm this charging effect, where a degenerated
semiconductor is used as the normal-metal wire. The proximity correction can be
picked from the entire conductance as the magnetoconductance of an
interferometer, and the charging effect is depicted by a gate control of the
superconducting island. The semiconductor interferometer is more promising than
a metallic one because the conductance without the proximity effect is bigger.
122. H. Namatsu
"Supercritical
drying for water-rinsed resist systems"
J.
Vac. Sci. Technol. B 18 (6), 3308-3312 (2000).
ABSTRACT: Two
methods of supercritical resist drying (SRD) using CO2 have been developed for
water-rinsed resist patterns. The key to their effectiveness is the use of a
surfactant. In indirect SRD, a solution of n-hexane, a CO2-philic liquid, and a
surfactant, sorbitan fatty acid ether, first replaces the water, and is in turn
replaced with liquid CO? before SRD is performed. The addition of a compound
with a high hydrophilic-lipophilic balance to the surfactant compensates for
the poor miscibility of water in a solution of n-hexane and sorbitan fatty acid
ether. In direct SRD, which does not require a CO2-philic liquid, the water is
replaced directly with liquid CO2 containing a surfactant, fluoroether
carboxylate, which makes water miscible in CO2; and then SRD is performed. The
excellent results Obtained by both methods demonstrate that there is no
inherent barrier to the use of SRD on water-rinsed resist patterns. (C) 2000
American Vacuum Society. [S0734-211X(00)01406-2].
123. H. Namatsu, K. Yamazaki,
and K. Kurihara
"Supercritical
resist dryer"
J.
Vac. Sci. Technol. B 18 (2), 780-784 (2000).
ABSTRACT: We
have developed a supercritical resist dryer in which resist patterns are
developed and successively dried with a supercritical fluid. The usage of
supercritical fluid in pattern drying is most effective for preventing pattern
collapse, which is a significant problem in fine patterning of less than 100 nm
critical dimensions. The key to performing ideal supercritical resist drying is
the prevention of water contamination due to moisture in the dryer chamber.
This is because the moisture dissolved in the supercritical fluid causes
pattern deformation which results from film swelling. As a technique to prevent
water contamination, we have devised pressure-controlled supercritical drying
where a supercritical fluid is sent pressurized to a Teflon coated chamber at
near the critical point. The supercritical resist dryer made on the basis of
this technique is an essential apparatus for next-generation lithography. (C)
2000 American Vacuum Society. [S0734-211X(00)01302-0].
124. K. G. Nath, F. Maeda, S.
Suzuki, and Y. Watanabe
"Epitaxy,
modification of electronic structures, overlayer-substrate reaction and
segregation in ferromagnetic Co films on Se-treated GaAs(001) surface"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 39
(7B), 4571-4574 (2000).
ABSTRACT: The
electronic structure and chemical states of the overlayer and substrate in
epitaxially grown Co films on Se-treated GaAs(001) 2 x 1 are investigated by
photoemission spectroscopy (PES) using synchrotron radiation. Adatom
(Co)-substrate (Ga) intermixing is found at the initial stages of Co
deposition. The intermixed layer is then buried and epitaxial growth is
achieved following further deposition. During the intermixing, Se is floated
over the surface of Co overlayers. A small amount of As-segregation is also
observed in the thicker Co films.
125. T. Nishida and N.
Kobayashi
"Nucleation
control in MOVPE of group III-nitrides on SiC substrate"
J.
Cryst. Growth 221, 297-300 (2000).
ABSTRACT: We
characterized nitride growth on SiC substrates by using surface sensitive in
situ monitoring of shallow angle reflectance (SAR). The growth initiation of
the AIN wetting layer on SiC substrate, and that of GaN on the AIN wetting
layer are studied, flat growth of the AIN wetting layer on SiC substrate is
achieved by excess source supply at the start. and the growth evolution of GaN
on the AIN wetting layer depends not only on the source flow rate but also on
the species of metalorganic source. Flat GaN and AlN wetting layer growth is
achieved by intentional nucleation. (C) 2000 Elsevier Science B.V. All rights
reserved.
126. J. Nitta, F. Meijer, Y.
Narita, and H. Takayanagi
"Gate
voltage-dependent Aharanov-Bohm experiment in the presence of Rashba spin-orbit
interaction"
Physica
E 6 (1-4), 318-321 (2000).
ABSTRACT: We
measured gate voltage-dependent Aharonov-Bohm oscillations in an InGaAs-based
two-dimensional electron gas ring with a gate on top of one of the branches.
After ensemble averaging, the h/e oscillation spectrum showed smooth
oscillatory behavior as a function of the gate voltage. This could be a
manifestation of the spin-orbit interaction induced interference. (C) 2000
Elsevier Science B.V. All rights reserved.
127. O. Niwa, R. Kurita, K.
Hayashi, T. Horiuchi, K. Torimitsu, K. Maeyama, and K. Tanizawa
"Continuous
measurement of histamine from rat basophilic leukemia cells (RBL-2H3) with an
on-line sensor using histamine oxidase"
Sens.
Actuator B-Chem. 67 (1-2), 43-51 (2000).
ABSTRACT:
Histamine release from rat basophilic leukemia (RBL-2H3) cells was continuously
measured using a histamine oxidase (HO)-immobilized on-line electrochemical
sensor. The sensor has a carbon-based electrode modified with a bilayer of
osmium-polyvinylpynidine-based gel containing horseradish peroxidase (HRP) and
BSA containing HO. The high specificity of the enzyme made the sensor highly
selective with regards to diamines such as putrescine and cadaverine. We
obtained a low detection limit of 23 nM owing to the low operation potential of
the sensor (below 0 V vs. Ag/AgCl) and the high activity of the enzyme after
immobilization. Moreover, the sensor had a high conversion efficiency. The
sensor response was unaffected by 400 min of continuous histamine measurement
and by more than 2 weeks of storage in a refrigerator. We combined the
histamine sensor with a microdialysis (MD) sampling probe and used it to
measure the histamine concentration of RBL-2H3 cells stimulated with
dinitrophenylated bovine serum albumin (DNP-BSA) after incubation with IgE. We
also fabricated a small volume histamine sensor by the microfabrication
technique and were able to measure the histamine release from a small mast cell
colony in real time with the sensor by drawing the extracellular solution
continuously through a sampling capillary located near the cells. (C) 2000
Elsevier Science S.A. All rights reserved.
128. O. Niwa, R. Kurita, Z. M.
Liu, T. Horiuchi, and K. Torimitsue
"Subnanoliter
volume wall-jet cells combined with interdigitated microarray electrode and
enzyme modified planar microelectrode"
Anal.
Chem. 72 (5), 949-955 (2000).
ABSTRACT:
Miniaturized wall-jet type flow cells with an active volume of 0.042 - 15 nL
were fabricated for use as highly sensitive electrochemical detectors for
capillary electrophoresis/electrochemical detection and small on-line enzyme
sensors. The cells consisted of three glass plates and a fused-silica
capillary. Two of the plates had microfabricated now channels and guide
trenches for the capillary and working, reference, and counter electrodes. The
other plate had a film electrode, When an interdigitated microarray electrode
(total area, 66 mu m x 64 mu m; bandwidth and gap, 2 mu m) was installed in the
now cell, the redox cycling enhanced the current at flow rates of less than 100
nL/min even though there were only eight pairs of microbands. A sharp dopamine
peak enhanced by the redox cycling was observed when the cell was used for
capillary electrophoresis, A square film electrode modified with glutamate
oxidase and Os-poly(vinylpyridine) containing HRP was also installed in the now
cell and used to measure neurotransmitter release from cultured nerve cells.
When the now rate was relatively high, the response time of the modified
electrode was comparable to that of a cylindrical carbon fiber electrode (33 mu
m o.d.) modified with the same enzyme and mediator. We observed a transient
cathodic current response assigned to the glutamate release with the electrode
in the flow cell in a suction mode measurement when we stimulated cultured
nerve cells electrically with a dual microelectrode.
129. H. Noda, T. Urisu, Y.
Kobayashi, and T. Ogino
"Initial
stage of hydrogen etching of Si surfaces investigated by infrared reflection
absorption spectroscopy"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 39
(12B), 6985-6989 (2000).
ABSTRACT: The
initial stage of etching reactions (breaking the Si-Si back bonds) of Si(100)
and Si(111) surfaces exposed to hydrogen at room temperature was investigated
by buried metal layer-infrared reflection absorption spectroscopy. The peaks of
SiH2 scissors and SiH3 deformation modes (<1000 cm(-1)) were successfully
observed as clear indicators of the initial stage of hydrogen etching
reactions. On the Si(100) surface. the hydrogen exposure dependence of these
peaks indicated that the etching reaction stal ts in the relatively
low-exposure region of <greater than or equal to>300L (1 L = 1 x 10(-6)
Torr s). We found that the adjacent dihydride is a precursor to breaking the Si
back bonds. On the Si(111) surface, it was found that the adatom's two back bonds
are easily broken, and that adatom trihydride is generated at a low H-exposure
of 70-500 L. Adding to this dominant reaction, the etching of the rest-atom
layer was observed at H-exposures higher than 10000 L.
130. S. Nojima
"Photonic-crystal
laser mediated by polaritons"
Phys.
Rev. B 61 (15), 9940-9943 (2000).
ABSTRACT: A
polariton-mediated photonic-crystal laser is proposed, which has a periodic
structure containing excitonic and gain materials in its unit cell. This type
of structure is shown to significantly intensify optical gain near the
polaritonic band edge as a result of using a light, the band of which is split
into small polaritonic bands by exciton-photon coupling. Consequently, this
laser exhibits much lower threshold gain than those of other lasers studied
here and it oscillates in the single mode because of its strong mode
selectivity. These advantages stem from the photon field modulated extremely by
adding excitons to conventional photonic crystals.
131. M. Notomi
"Theory
of light propagation in strongly modulated photonic crystals: Refractionlike
behavior in the vicinity of the photonic band gap"
Phys.
Rev. B 62 (16), 10696-10705 (2000).
ABSTRACT:
Although light propagation in weakly modulated photonic crystals is basically
similar to propagation in a diffraction grating in which conventional
refractive index loses its meaning, we demonstrate that light propagation in
strongly modulated two-dimensional (2D)/3D photonic crystals becomes
refractionlike in the vicinity of the photonic bandgap. Such a crystal behaves
as a material having an effective refractive index controllable by the band
structure. This situation is analogous to the effective-mass approximation id
electron-band theory. By utilizing this phenomenon, negatively refractive material
can be realized, which has interesting optical properties such as mirror-image
refraction.
132. M. Notomi, T. Tamamura, T.
Kawashima, and S. Kawakami
"Drilled
alternating-layer three-dimensional photonic crystals having a full photonic
band gap"
Appl.
Phys. Lett. 77 (26), 4256-4258 (2000).
ABSTRACT: We
propose a three-dimensional photonic crystal structure having a wide full
photonic band gap in the optical regime, which can be fabricated by an
alternating-layer deposition and etching (drilling) process. This fabrication
process is much simpler than that previously reported. The combination of
current lithographic technology and autocloning bias-sputtering deposition is a
promising way of realizing these photonic crystals. (C) 2000 American Institute
of Physics. ([)S0003-6951(00)03451-3].
133. M. Notomi, T. Tamamura, Y.
Ohtera, O. Hanaizumi, and S. Kawakami
"Direct
visualization of photonic band structure for three-dimensional photonic
crystals"
Phys.
Rev. B 61 (11), 7165-7168 (2000).
ABSTRACT: We
propose a method to experimentally determine the full photonic band structure
of photonic crystals by monitoring the beam propagation, and we demonstrate the
experimental results of the band-structure measure ment in the near-infrared
regime for Si/SiO2 three-dimensional hexagonal photonic crystals fabricated by
autocloning bias-sputtering process.
134. S. Nuttinck, K. Hashimoto,
S. Miyashita, T. Saku, Y. Yamamoto, and Y. Hirayama
"Quantum
point contacts in a density-tunable two-dimensional electron gas"
Jpn.
J. Appl. Phys. Part 2 - Lett. 39 (7A), L655-L657 (2000).
ABSTRACT:
Quantum point contacts fabricated using a backgated two-dimensional
electron-gas system show clear quantized features and a 0.7 anomaly in
conductance. Using these density-tunable point contacts, we have studied the
behavior of the 0.7 anomaly. The 0.7 step shifts down to around 0.5 as the
electron density is decreased under a zero magnetic field. This suggests that
electron-electron interactions play an important role in forming the
conductance anomalies of quantum point contacts.
135. A. A. Odintsov and Y.
Tokura
"Contact
phenomena in carbon nanotubes"
Physica
B 284, 1752-1753 (2000).
ABSTRACT:
Poor screening of the long-range Coulomb interaction in one-dimensional carbon
nanotubes results in a peculiar picture of contact phenomena. Being brought to
a contact with a metal, conducting nanotube accumulates electric charge whose
density decays slowly with the distance from the contact. This should be
contrasted to a conventional metal-metal contact where the charge density
decreases exponentially at atomic distances. Implications for experiments are
discussed. (C) 2000 Elsevier Science B.V. All rights reserved.
136. A. A. Odintsov and Y.
Tokura
"Contact
phenomena and Mott transition in carbon nanotubes"
J.
Low Temp. Phys. 118 (5-6), 509-518 (2000).
ABSTRACT: We
describe the transfer of electric charge in junctions between a metal and
carbon nanotube as well as between metallic and semiconducting carbon
nanotubes. The long range Coulomb interaction drastically modifies the charge
transfer phenomena in one-dimensional nanotube systems compared to conventional
semiconductor heterostructures. Being brought into a contact with a metal,
conducting nanotube accumulates electric charge whose density decays slowly
with the distance from the junction. The length of the Schottky barrier in
nanotube heterojunctions varies from the distances of the order of the nanotube
radius (nanometers) to the distances of the order of the nanotube length
(microns) depending on a doping strength. The Schottky barrier height shows
pronounced asymmetry under the forward and reverse bias. This results in
rectifying behavior of heterojunctions, in agreement with recent experimental
observations by Z. Yao et. al. and P. McEuen et. al. Finally, we discuss
observability of recently predicted Mott insulating phase in metallic carbon
nanotubes.
137. H. Ofuchi, T. Kubo, M.
Tabuchi, K. Takahei, and Y. Takeda
"Local
structures around Er atoms in GaAs: Er,O studied by fluorescence EXAFS and
photoluminescence"
Microelectron.
Eng. 51-2, 715-721 (2000).
ABSTRACT: We
have investigated Er- and O-doped GaAs samples by fluorescence extended X-ray
absorption fine structure (EXAFS) measurements in order to clarify the local
structures around the Er atoms. The EXAFS analysis revealed that in the range
of Er concentration from 2 X 10(18) cm(-3) to 3 X 10(20) cm(-3) the majority of
the Er atoms substituted Ga sublattice with two adjacent oxygen atoms (Er-2O
center). On the contrary, in the same range of the Er concentration the PL
intensity decreased rapidly with the increase of the Er concentration. The
EXAFS analysis also indicated that the averaged arrangements of second or third
neighbor atoms are different in each sample. Therefore, the Er-2O centers are
considered to be further modified by the local structures of those second and
even third nearest neighbors, which in turn change their optical
characteristics. (C) 2000 Elsevier Science B.V. All rights reserved.
138. T. Ogino, Y. Homma, H.
Hibino, Y. Kobayashi, P. Kuniyil, K. Sumitomo, H. Omi, and P. Finnie
"Control
of Si surfaces for fabrication of integrated functional nanostructures"
Abstr.
Pap. Am. Chem. Soc. 219, U343-U343 (2000).
ABSTRACT:
139. K. Oguri, N. Funamori, T.
Uchida, N. Miyajima, T. Yagi, and K. Fujino
"Post-garnet
transition in a natural pyrope: a multi-anvil study based on in situ X-ray
diffraction and transmission electron microscopy"
Phys.
Earth Planet. Inter. 122 (3-4), 175-186 (2000).
ABSTRACT:
Post-garnet transition in a natural pyrope under the conditions close to 670 km
discontinuity was studied by in situ X-ray diffraction (XRD) using an MA8-type
multi-anvil apparatus and analytical transmission electron microscopy (ATEM) on
recovered samples. The pyrope with a composition of
(Mg0.72Fe0.17Ca0.11)(3)Al2Si3O12 directly breaks down into (Mg, Fe)SiO3-Al2O3
perovskite, CaSiO3 perovskite, stishovite, and the 'NAL' phase with increase in
density of about 10%. The presence of the 'NAL' phase that was first discovered
in the diamond-anvil cell (DAC) experiments was confirmed by multi-anvil
experiments. The transition boundary can be expressed as P (GPa) = 14.4 +
0.0065T (K) between 1200 and 2000 K, suggesting that, below 1400 K, the
transition pressure may be lower than 24 GPa, the pressure corresponds to the
670 km discontinuity. These results, together with available information on
garnets with various compositions, suggest that chemical compositions of
garnets strongly affect both transition conditions and post-garnet
high-pressure mineral assemblages. (C) 2000 Elsevier Science B.V. All rights
reserved.
140. K. Okajima, K. Takeda, N.
Oyama, E. Ohta, K. Shiraishi, and T. Ohno
"Phenomenological
theory of semiconductor epitaxial growth with misfit-dislocations"
Jpn.
J. Appl. Phys. Part 2 - Lett. 39 (9AB), L917-L920 (2000).
ABSTRACT: We
have developed a phenomenological theory of growth behavior in semiconductor
heteroepitaxy that includes the effects of the formation of Stranski-Krastanov
(SK) islands and misfit-dislocations (MDs). Our theory can reproduce the
various types of growth behavior observed in hereroepitaxial growth. Moreover,
we also formulate a procedure for determining the phenomenological parameters
that includes atomistic calculations. The critical thickness of InAs/GaAs(110)
obtained by this procedure is in good agreement with the experimentally
obtained value.
141. H. Omi and T. Ogino
"Growth-induced
atomic step ordering on patterned and non-patterned Si(111)"
Thin
Solid Films 380 (1-2), 15-19 (2000).
ABSTRACT:
Atomic step configurations on the vicinal surfaces of patterned and
non-patterned Si(111) during homoepitaxial step-flow growth were studied as a
function of film thickness, deposition temperature, deposition rate, and
substrate miscut. We found, for the first time, that step-flow growth on the
vicinal surfaces of Si(111) miscut toward the [11 (2) over bar] direction
results in the formation of collective, in-phase zigzag arrays of [2 (11) over
bar]- and [(1) over bar2 (1) over bar]-type steps. We also found that step-flow
growth on the lower-level region around the edge of Si(111) mesa ridges
significantly improves period uniformity. We explained the shape of atomic
steps on the basis of the stability of surface reconstruction on Si(111), and
the atomic step ordering on the assumption of the anisotropic barrier for
diffusion at the growing steps. (C) 2000 Elsevier Science B.V. All rights
reserved.
142. H. Omi and T. Ogino
"Positioning
of self-assembling Ge islands on Si(111) mesas by using atomic steps"
Thin
Solid Films 369 (1-2), 88-91 (2000).
ABSTRACT:
Atomic steps were rearranged during step-flow growth of Si epitaxial layers on
0.6- and 1.5-mu m-wide Si(111) mesas oriented in the [11 (2) over bar]
direction during molecular beam epitaxy. Ge islands were then grown on the mesa
tops to form well-positioned arrays of self-assembling nanodots. On the 0.6-mu
m-wide mesas, the Si growth produced arrays of arrowheads composed of [(1) over
bar (1) over bar 2]-type bunched steps. Ge islands preferentially grow at the
vertices of arrowhead-like steps, aligning along the center of a mesa. On
1.5-mu m-wide mesas, on the other hand, the resulting steps have a
zigzag-shaped pattern and Ge islands also preferentially grow at the vertices
of zigzag steps. These results demonstrate that by using atomic steps with
artificially designed arrangement, it is possible to position and align the Ge
islands on Si(111) mesas. (C) 2000 Elsevier Science S.A. All rights reserved.
143. Y. Ono, Y. Takahashi, K.
Yamazaki, M. Nagase, H. Namatsu, K. Kurihara, and K. Murase
"Single-electron
transistor and current-switching device fabricated by vertical pattern-dependent
oxidation"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 39
(4B), 2325-2328 (2000).
ABSTRACT:
Vertical pattern-dependent oxidation, a method of fabricating single-electron
transistors, has been advanced so that it can be applied to make various types
of single-electron logic circuits. The improved method changes the pattern of
Si to be oxidized from the original. Using the improved method, we have
demonstrated a single-electron transistor with a new structure and a current-switching
device composed of the new single-electron transistors.
144. Y. Ono, Y. Takahashi, K.
Yamazaki, M. Nagase, H. Namatsu, K. Kurihara, and K. Murase
"Si
complementary single-electron inverter with voltage gain"
Appl.
Phys. Lett. 76 (21), 3121-3123 (2000).
ABSTRACT: A
Si complementary single-electron inverter in which two identical
single-electron transistors (SETs) are packed is fabricated on a
silicon-on-insulator substrate. For the fabrication, the vertical
pattern-dependent oxidation method, which enables the formation of two tiny
SETs aligned in parallel, is modified so that the two SETs can be connected in
series to realize an inverter configuration. The resultant circuit occupies a
very small area: 100x100 nm for each SET. For complementary operation, the
electrical characteristics of one of the SETs are shifted using a side gate
situated near the SET. Input-output transfer with a voltage gain larger than
unity is demonstrated at 27 K. (C) 2000 American Institute of Physics.
[S0003-6951(00)04821-X].
145. Y. Ono, Y. Takahashi, K.
Yamazaki, M. Nagase, H. Namatsu, K. Kurihara, and K. Murase
"Fabrication
method for IC-oriented Si single-electron transistors"
IEEE
Trans. Electron Devices 47 (1), 147-153 (2000).
ABSTRACT: A
new fabrication method for Si single-electron transistors (SET's) is proposed,
The method applies thermal oxidation to a Si wire with a fine trench across it
on a silicon-on-insulator substrate. During the oxidation, the Si wire with the
fine trench is converted, in a self-organized manner, into a twin SET structure
with two single-electron islands, one along each edge of the trench, due to
position-dependent oxidation-rate modulation caused by stress:accumulation.
Test devices demonstrated, at 40K, that the twin SET structure can operate as
two individual SET's. Since the present method produces two SET's at the same
time in a tiny area, It is suitable for integrating logic circuits based on
pass-transistor-type logic and CMOS-type logic, which promises to lead to the
fabrication of single-electron logic LSI's.
146. K. Prabhakaran, F. Maeda,
Y. Watanabe, and T. Ogino
"Thermal
decomposition pathway of Ge and Si oxides: observation of a distinct
difference"
Thin
Solid Films 369 (1-2), 289-292 (2000).
ABSTRACT: In
this paper, we report a comparison of the thermal decomposition pathways of
ultrathin oxide layers, formed on Ge(100) and Si(100) surfaces, as revealed by
photoemission studies, employing synchrotron radiation. The oxide layer, in
both the cases, consists of a mixture of, mainly, monoxide and dioxide species.
On annealing, both the oxides undergo thermal decomposition and the desorbing
species is the corresponding monoxide. However, we find that their
decomposition pathways are entirely different. On annealing the Ge oxide layer,
the GeO2 species transforms to GeO on the surface and finally desorbs from the
surface at similar to 425 degrees C. In contrast, annealing results in the
transformation of SiO to SiO2 up to a temperature, lower than the desorption
temperature (similar to 760 degrees C). At higher temperatures, SiO2 possibly
transforms back to SiO and subsequently desorbs. These phenomena may be related
to the interface properties, since the thermodynamic properties of individual
oxides predict an opposite trend in their thermal stability. (C) 2000 Elsevier
Science S.A. All rights reserved.
147. K. Prabhakaran, F. Maeda,
Y. Watanabe, and T. Ogino
"Distinctly
different thermal decomposition pathways of ultrathin oxide layer on Ge and Si
surfaces"
Appl.
Phys. Lett. 76 (16), 2244-2246 (2000).
ABSTRACT: The
thermal decomposition pathway of an ultrathin oxide layer on Ge(100) and
Si(100) surfaces is examined by synchrotron radiation photoelectron
spectroscopy and ultraviolet photoelectron spectroscopy with helium I
radiation. The as-prepared oxide layer consists of a mixture of oxides, namely,
suboxides and dioxides, on both the surfaces. Upon annealing, the oxide layers
decompose and desorb as monoxides. However, we find that the decomposition
pathways are different from each other. On annealing Ge oxides, GeO2 species
transform to GeO and remain on the surface and desorb at > 420 degrees C. In
contrast, annealing of Si oxides results in the transformation of SiO to SiO2 up
to temperatures (similar to 780 degrees C) close to the desorption. At higher
temperatures, SiO2 decomposes and desorbs, implying a reverse transformation to
volatile SiO species. (C) 2000 American Institute of Physics.
[S0003-6951(00)04816-6].
148. K. Prabhakaran, K.
Sumitomo, and T. Ogino
"Nano-interface
engineering of Co/Ge/Si systems: metal incorporation into Ge quantum dots and
SiO2/Si structures"
Appl.
Surf. Sci. 159, 492-497 (2000).
ABSTRACT: In
this paper, we describe the nano-interface engineering of Co/Ge/Si system,
involving interface reactions. Controlled annealing causes the Co atoms to
diffuse through an already formed quantum dot network fabricated on a silicon
substrate and get incorporated as epitaxial CoSi2. Additionally, we performed in
situ examination of the early stages of oxide mediated epitaxial growth of
Silicide at the SiO2/Si interface on a Si surface. Cobalt, deposited at room
temperature on an SiO2 layer. diffuses through the oxide layer and forms
epitaxial CoSi2 at the interface, preserving the original oxide surface
morphology. These results suggest the possibility of an alternative and viable
method to introduce functionality into nanostructures. (C) 2000 Elsevier
Science B.V. All rights reserved.
149. J. H. Roslund, K. Saito,
K. Suzuki, H. Yamaguchi, and Y. Hirayama
"Electron
and hole proximity effects in the InAs/AlSb/GaSb system"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 39
(4B), 2448-2451 (2000).
ABSTRACT: We
have investigated the properties of InAs/AlSb/GaSb electron-hole proximity
systems while focusing on the influence of the AlSb barrier between the two
quantum wells. We have seen that for thin AlSb barriers there is a drop in
mobility due to scattering of electrons by holes. We have also observed a
series of secondary absorption peaks in cyclotron resonance spectra that are
caused by interband Landau-level transitions.
150. J. H. Roslund, H.
Yamaguchi, and Y. Hirayama
"Electrical
properties of InAs/AlSb/GaSb double quantum well structures"
in
Compound Semiconductors 1999, Institute Of Physics Conference Series
Vol. 166 (Iop Publishing Ltd, Bristol, 2000), pp. 127-130.
ABSTRACT: The
electrical properties of InAs/AlSb/GaSb double quantum well structures have
been investigated and the InAs/AlSb interfaces were seen to be responsible for
changing the balance between electrons and holes, creating a surplus of
electrons.
151. M. S. M. Saifullah, K.
Kurihara, and C. J. Humphreys
"Comparative
study of sputtered and spin-coatable aluminum oxide electron beam resists"
J.
Vac. Sci. Technol. B 18 (6), 2737-2744 (2000).
ABSTRACT: The
electron beam exposure characteristics of sputtered AlOx and spin-coatable
Al2O3 resists are compared and contrasted. When exposed to an electron beam,
sputtered AlOx resists on a silicon substrate undergo an intense mass loss.
However, electron energy loss spectroscopy shows that even after a prolonged
exposure some aluminum and oxygen remains on the silicon surface. Spin-coatable
Al2O3 resist was prepared by reacting aluminum tri-sec-butoxide, Al(OBus)(3),
with acetylacetone (AcAc) in isopropyl alcohol. These are negative tone resists
and they are > 10(6) times more sensitive to an electron beam than the
sputtered AlOx, bringing its sensitivity very close to high resolution organic
resists such as calixarene. The exposure properties of spin-coatable and
sputtered aluminum oxide resists are discussed together with their sensitivity,
damage mechanisms, line edge roughness, and etching characteristics. A brief
note on the change of methodology of resist design is added when inorganic
resists are to be used in high resolution electron beam nanolithography. (C)
2000 American Vacuum Society. [S0734-211X(00)15706-3].
152. T. Saitoh, T. Sogawa, M.
Notomi, T. Tamamura, S. Kodama, T. Furuta, and H. Ando
"GaAs
photonic crystals on SiO2 fabricated by very-high-frequency anode-coupled
reactive ion etching and wafer bonding"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 39
(11), 6259-6263 (2000).
ABSTRACT:
High-aspect-ratio, two-dimensional (2D) air-column GaAs photonic crystals
(PhCs) on SiO2 layers with a lattice constant ranging from 240 nm to 1.0 mum
have been fabricated using a novel method combining wafer bonding and low-temperature
very-high-frequency (VHF) reactive ion etching (RIE). The obtained PhCs exhibit
near-field patterns of sixfold symmetry or fourfold symmetry due to lateral
interference, depending on the lattice structure. We have obtained
photoluminescence (PL) spectra of PhCs which reveal the low damage feature of
the combined process of low-temperature RIE and wafer bonding. Reflectance
spectra exhibit fine structures which originate from the resonance coupling of
the external light to the zone-folded bands of the photonic structure. This
vertical confinement structure, obtained by forming GaAs PhCs on SiO2, is
useful for taking advantage of 2D photonic crystals since it prevents photon
dissipation from the lattice plane. The fabrication method combining low-temperature
RIE with wafer bonding is a promising process for developing 2D photonic
crystals on SiO2 layers.
153. S. Sasaki, S. De
Franceschi, J. M. Elzerman, W. G. van der Wiel, M. Eto, S. Tarucha, and L. P.
Kouwenhoven
"Kondo
effect in an integer-spin quantum dot"
Nature 405
(6788), 764-767 (2000).
ABSTRACT: The
Kondo effect-a many-body phenomenon in condensed-matter physics involving the
interaction between a localized spin and free electrons-was discovered in
metals containing small amounts of magnetic impurities, although it is now
recognized to be of fundamental importance in a wide class of correlated
electron systems(1,2). In fabricated structures, the control of single,
localized spins is of technological relevance for nanoscale electronics(3,4).
Experiments have already demonstrated artificial realizations of isolated
magnetic impurities at metallic surfaces(5,6), nanoscale magnets(7), controlled
transitions between two-electron singlet and triplet states(8), and a tunable
Kondo effect in semiconductor quantum dots(9-12). Here we report an unexpected Kondo
effect in a few-electron quantum dot containing singlet and triplet spin
states, whose energy difference can be tuned with a magnetic field. We observe
the effect for an even number of electrons, when the singlet and triplet states
are degenerate. The characteristic energy scale is much larger than in the
ordinary spin-1/2 case.
154. H. Sato, A. Tsukada, M.
Naito, and A. Matsuda
"La-214
thin films under epitaxial strain"
Physica
C 341, 1767-1770 (2000).
ABSTRACT:
Compressive (or expansive) epitaxial strain was induced in (001)-oriented
La-214 thin films. For the compressed films of La2-xSrxCuO4+delta and
La2-xBaxCuO4+delta on LaSrAlO4 substrates, the superconducting transition
temperature (T-c) reached 44 K and 47 K, respectively, with delta similar to0
When both films had delta > 0, T-c reached 49 K. These values are higher
than those for bulk samples. The T-c-x phase diagrams for the films did not
show a local minimum at x similar to 0.125, the so-called "1/8
anomaly". The compressive strain expands the c-axis via the Poisson effect
and suppresses formation of the low-temperature tetragonal phase. Both effects
result in an increase in the bond length between Cu and the apical oxygen
(O-apex), which is responsible for the enhancement of T-c Furthermore, based on
the experimental fact that the lower residual resistivity gives a higher T-c,
we speculate that the T-c enhancement is caused by the reduced
antiferromagnetic spin fluctuation in the CuO2 planes due to the change in the
Cu-O-apex bond length.
155. H. Sato, A. Tsukada, M.
Naito, and A. Matsuda
"Absence
of (1)/(8) anomaly in strained thin films of La2-xBaxCuO4+delta"
Phys.
Rev. B 62 (2), R799-R802 (2000).
ABSTRACT:
Compressive and expansive strain was induced into La2-xBaxCuO4+delta thin films
with x = 0-0.35 on LaSrAlO4 and SrTiO3 substrates, respectively. For the
compressed films, the superconducting transition temperature (T-c) reached 44 K
with delta similar to 0 and 49 K with delta>0, and the T-c-x phase diagram
did not show a local minimum at x similar to 0.125, the so-called "1/8
anomaly." For the expanded films, we observed strong reduction of T-c. We
suggest that the absence of the "1/8 anomaly" in the compressed films
is due to the c-axis expansion, as well as the in-plane compression, and
suppression of the residual resistivity.
156. H. Sato, A. Tsukada, M.
Naito, and A. Matsuda
"La2-xSrxCuOy
epitaxial thin films (x=0 to 2): Structure, strain, and superconductivity"
Phys.
Rev. B 61 (18), 12447-12456 (2000).
ABSTRACT: We
have grown (001)-oriented thin films of La2-xSrxCuOy with strontium composition
x=0-2 by reactive coevaporation and characterized them by x-ray-diffraction and
resistivity measurements. A systematical change in the c-axis length indicates
that single-phase films were obtained for the whole compositional range. The
films with the oxygen composition gamma similar to 4 showed superconductivity
for x between 0.06 and 0.30. For x=0.15, the superconducting transition
temperature (T-c) was maximized to 44 K, due to a strain effect caused by the
lattice mismatch between films and substrates. Around this composition, it is
found that T-c for the films shows a good correlation with the c-axis length.
For x=0.30, T-c for the films strongly depends on the residual resistivity [rho(0
K)]: higher T-c for lower rho(0 K). The depression of T-c around x=0.125 is
smaller than that for the bulk samples, suggesting that the strain suppresses
the "1/8 anomaly." The films with gamma>4 attained by cooling in
ozone showed T-c between 40 and 48 K for x<0.15. For x>0.30, the
compositional dependence of the resistivity is explained by both oxygen defects
and a structural phase transition at x=1.8.
157. C. Sekar, T. Watanabe, and
A. Matsuda
"Crystal
growth and characterization of the 4-leg spin ladder compound La2Cu2O5"
J.
Cryst. Growth 212 (1-2), 142-147 (2000).
ABSTRACT:
Crystallization of La2Cu2O5, has been investigated in the La2O3-CuO system for
various starting compositions both in air and oxygen atmospheres. In air, we
find that there exists a new region of crystallization of La8Cu7O19 phase, just
above that of La2Cu2O5. However, this region vanishes completely in
flowing-oxygen atmosphere. By utilizing this, large single crystals of the
4-leg spin-ladder compound La2Cu2O5 have been successfully grown from CuO flux
by the slow cooling method. Room-temperature resistivity parallel to the ladder
direction (\b) of the as-grown crystals is estimated to be 1.7 x 10(3) Ohm cm.
A significant decrease in the resistivity (798 m Ohm cm at 300 K) is observed
upon hole doping by means of high oxygen pressure annealing (approximately 400
atm) using a hot isostatic pressing furnace. However, no transition was
observed from the semiconducting behavior. (C) 2000 Elsevier Science B.V. All
rights reserved.
158. K. Semba, A. Matsuda, and
M. Mukaida
"Carrier-concentration-driven
superconductor-to-insulator transition in YBa2Cu3O6+x"
Physica
B 281, 904-905 (2000).
ABSTRACT: We
have succeeded in controlling carrier concentration near the
superconductor-to-insulator transition by sample annealing under the
equilibrium oxygen pressure of YBa2Cu3O6+x. Near the critical doping, below 60
K, we observed carrier-concentration-driven resistivity scaling of the:
pulsed-laser-deposited thin of YBa2Cu3O6+x indicating the large energy scale of
the quantum phase fluctuation. This demonstrates that a considerable area in
the phase diagram of the pseudo-gapped underdoped YBa2Cu3O6+x is in the
critical region of the quantum phase transition. (C) 2000 Published by Elsevier
Science B.V. All rights reserved.
159. R. Shaikhaidarov, A. F.
Volkov, H. Takayanagi, V. T. Petrashov, and P. Delsing
"Josephson
effects in a superconductor-normal-metal mesoscopic structure with a dangling
superconducting arm"
Phys.
Rev. B 62 (22), 14649-14652 (2000).
ABSTRACT: We
studied a mesoscopic crosslike normal-metal structure connected to two
superconducting (S) and two normal (N) reservoirs. We observed the Josephson
effect under unusual conditions when there is no current through one of the two
S/N interfaces. The potential difference between the S reservoirs was zero
unless the voltage applied between S and N reservoirs exceeded a critical value
although the electric potential in the N wire connecting the superconductors
varied in a nonmonotonic way. The observed effects are discussed theoretically.
160. K. Shimizu and N. Imoto
"Single-photon-interference
communication equivalent to Bell-state-basis cryptographic quantum
communication"
Phys.
Rev. A 62 (5), art. no.-054303 (2000).
ABSTRACT: We
propose a single-photon interferometer which provides cryptographic quantum
communication equivalent to that obtained using a pair of polarization
entangled photon twins as a carrier [Phys. Rev. A 60, 157 (1999)]. Instead of
manipulating and measuring the internal states of entangled photon twins,
cryptographic quantum communication is possible by manipulating a single photon
in an extended interferometer. The use of the single-photon interferometer
offers significant experimental advantages compared to our previous approach.
161. K. Shimizu and N. Imoto
"Quantum
information processing - Quantum cryptography toward ultimate security"
Ntt
Rev. 12 (1), 26-31 (2000).
ABSTRACT:
Recent progress in digital computer communication networks has increased the
awareness of the importance of information security technologies for private
communications, message authentication, and data protection. NTT Basic Research
Laboratories is pushing towards the realization of quantum cryptography, an
innovative new concept of cryptography based on the principles of quantum
mechanics. If a quantum cryptographic system can be successfully developed,
there will be absolutely no possibility of security violations in private
communications.
162. M. Shimoda, S. Tsukamoto,
T. Ohno, N. Koguchi, M. Sugiyama, S. Maeyama, and Y. Watanabe
"Stoichiometry
study of S-terminated GaAs(001)-(2 x 6) surface with synchrotron radiation
photoelectron spectroscopy"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 39
(7A), 3943-3946 (2000).
ABSTRACT:
Synchrotron radiation photoelectron spectroscopy (SRPES) has been performed to
investigate the surface stoichiometry of the S-terminated GaAs(001)-(2 x 6),
and in particular, to determine the chemical species of the five dimers, which
are separated by missing dimers and from the unit structure of the (2 x 6)
reconstruction. The S 2p photoemission spectra show a significant decrease in
the peak intensity with increasing substrate temperature, whereas no
significant changes are observed for the As 3d photoemission spectra The Ga 3d
spectra are decomposed into a bulk component and more than one surface
component, one of which is attributed to a Ga-S bond and decreases in
accordance with the change observed in the S 2p spectra. These results strongly
support the model that each pair of the five dimers in the (2 x 6)
reconstruction consists of S-S dimers.
163. D. J. Shin, A.
Chavez-Pirson, and Y. H. Lee
"Multipole
analysis of the radiation from near-field optical probes"
Opt.
Lett. 25 (3), 171-173 (2000).
ABSTRACT: We
experimentally and theoretically analyze the radiation emitted from
subwavelength-sized apertures in nearfield optical probes. By decomposing the
experimentally obtained radiation patterns into vector spherical waves, we
describe the fields in terms of a series of multipole sources. We fit
polarization-resolved angular intensity distributions, measured as far as 150
degrees from the normal, with dipole, quadrupole, and octupole radiation. We
find that the magnetic and the electric dipole components are dominant but that
the interference terms between dipoles and higher-order poles are not
negligible. This result can be used as the basis for understanding near-field
optical interactions and images. (C) 2000 Optical Society of America. OCIS codes:
260.1960, 180.5810.
164. K. Shiraishi, H.
Kageshima, and M. Uematsu
"Phenomenological
theory on Si layer-by-layer oxidation with small interfacial islands"
Jpn.
J. Appl. Phys. Part 2 - Lett. 39 (12B), L1263-L1266 (2000).
ABSTRACT: We
theoretically investigate the mechanism of Si layer-by-layer oxidation by
taking into account interfacial Si emission. Based on the free energy
expression, which includes the oxidation-induced strain within the elastic
continuum theory, we simulated the oxidation. Initially, oxidation occurs at
the step edge of the interface. However, it stops because of the accumulated
strain, and the oxidation at the terrace region begins. As a result, many small
islands form at the interface. After their formation, the Si emission occurs to
release the interfacial strain. Accordingly, oxidation at the step edges of the
small islands becomes possible due to the strain release by Si emission. This
process is qualitatively in good agreement with recent observations of Si
layer-by-layer oxidation concurrent with the formation of many small oxide
islands.
165. K. Shiraishi, M. Nagase,
S. Horiguchi, H. Kageshima, M. Uematsu, Y. Takahashi, and K. Murase
"Designing
of silicon effective quantum dots by using the oxidation-induced strain: a theoretical
approach"
Physica
E 7 (3-4), 337-341 (2000).
ABSTRACT: We
have investigated using partial oxidation of an Si wire for forming quantum
dots. Calculated results show oxidation induced strain leads to the formation
of effective quantum dots, although actual dot-shaped structures are not
formed. By investigating formation conditions, we have found that partial
oxidation of an Si wire on a (0 0 1) substrate is very efficient for the
formation of oxidation-induced effective quantum dots. Moreover, our calculated
results are qualitatively consistent with experimental results obtained with
our Si single-electron transistors (Si-SET) fabricated by pattern-dependent
oxidation (PADOX). (C) 2000 Elsevier Science B.V. All rights reserved.
166. T. Sogawa, H. Ando, and S.
Ando
"Spin
relaxation dynamics of drifting electrons in GaAs narrow (10 nm) quantum
wires"
in
Compound Semiconductors 1999, Institute Of Physics Conference Series
Vol. 166 (Iop Publishing Ltd, Bristol, 2000), pp. 223-226.
ABSTRACT: We
investigated drift and diffusion dynamics of optically spin-polarized electrons
in p-type rectangular GaAs/AlAs quantum wires with small (10 nm) lateral sizes
by time- and spatially-resolved photoluminescence measurement. It is revealed
that the drift process rapidly expands the spin-polarized electrons and that
the spin polarization is maintained beyond 10 mum. The spin-reserved transport
is probably due to the suppressed scattering between the spin-polarized
electrons in a narrow one-dimensional channel.
167. T. Sogawa, H. Ando, and S.
Ando
"Drift
and diffusion dynamics of optically spin-polarized electrons in GaAs quantum
wires"
Physica
E 7 (3-4), 1020-1024 (2000).
ABSTRACT: We
investigated drift and diffusion dynamics of optically spin-polarized electrons
in rectangular p-doped GaAs/AlAs quantum wires (QWRs) with small (10 nm)
lateral sizes by time resolved and spatially resolved photoluminescence
measurement. It is revealed that the drifting electrons tend to maintain the
spin polarization beyond 10 mu m, while the diffusion process causes the
spatially-uniform spin relaxation with a spin relaxation time of about 300 ps.
(C) 2000 Elsevier Science B.V. All rights reserved.
168. T. Sogawa, H. Ando, and S.
Ando
"Spin-transport
dynamics of optically spin-polarized electrons in GaAs quantum wires"
Phys.
Rev. B 61 (8), 5535-5539 (2000).
ABSTRACT: We
investigate the drift and diffusion dynamics of optically spin-polarized
electrons in p-type rectangular GaAs/AlAs quantum wires with small (10 nm) lateral
sizes by time- and spatially resolved photoluminescence measurement. The drift
process causes a rapid expansion of the spin-polarized electrons, keeping the
spin polarization beyond by 10 mu m. We theoretically analyze the transport
characteristics of spin-polarized electrons and their spin-relaxation dynamics
based on a drift-diffusion model which includes a spin-flip process; Experiment
can be consistently explained by considering that the dependence of the
diffusivity and mobility on the degree of the spin polarization, demonstrating
the possibility of spin-dependent electron-electron scattering that affects the
transport properties in one-dimensional structures.
169. G. S. Solomon, M. Pelton,
and Y. Yamamoto
"Spontaneous
emission control of single quantum dots"
in
Compound Semiconductors 1999, Institute Of Physics Conference Series
Vol. 166 (Iop Publishing Ltd, Bristol, 2000), pp. 269-272.
ABSTRACT:
Modification of the spontaneous emission properties of a single InAs quantum
dot is demonstrated using a epitaxial distributed-Bragg reflector microcavity
that has been processed into posts with diameters ranging in size from 20 mum
to 0.5 mum. The micropost structure isolates single quantum dots within the
microcavity resonance, and creates a 3-dimensionally (3D) confined optical
cavity. The discrete mode structure of the 3D cavity is observed, as well as
the coupling of a single quantum dot to one of these modes in the weak coupling
cavity QED regime.
170. G. S. Solomon, M. Pelton,
and Y. Yamamoto
"Modification
of spontaneous emission of a single quantum dot"
Phys.
Status Solidi A-Appl. Res. 178 (1), 341-344 (2000).
ABSTRACT:
Modification of spontaneous emission of a single InAs quantum dot is
demonstrated using an epitaxial distributed Bragg reflector microcavity that
has been post-growth processed into microposts. The micropost structure
isolates single quantum dots within the microcavity resonance, and creates a
three-dimensionally (3D) confined photonic cavity. Discrete mode structure from
the 3D cavity is observed, as well as the coupling of a single quantum dot to
one of these modes in the weak coupling cavity QED regime.
171. O. M. Stoll, R. P.
Huebener, S. Kaiser, and M. Naito
"Electric
field dependence of the flux-flow resistance and the electronic vortex
structure in the cuprate superconductor Nd2-xCexCuOy"
J.
Low Temp. Phys. 118 (1-2), 59-74 (2000).
ABSTRACT: In the
temperature limit T much less than T-c c-axis oriented films of the cuprate
super-conductor Nd2-xCexCuOy display an intrinsic step structure of the
flux-flow resistance. Under current bias hysteretic voltage steps appear,
whereas under quasi voltage bias negative differential resistance (NDR) is
observed. For explaining these instabilities, we propose an electronic
structure in the mixed state, consisting of subbands between the Fermi energy
and the superconducting energy gap. The subbands originate from the Andreev
bound states in the core of an isolated vortex, because of the interaction
between vortices. Bloch oscillations of the quasiparticles in the narrow
subbands are proposed as the mechanism generating the NDR.
172. O. M. Stoll, A. Wehner, R.
P. Huebener, and M. Naito
"Negative
differential flux-flow resistance and relaxation oscillations in the cuprate
superconductor Nd2-xCexCuOy"
Physica
B 284, 827-828 (2000).
ABSTRACT: We
report on measurements of the flux-flow resistance in Nd2-xCexCuOy under
voltage bias and present a model for the observed relaxation oscillations. (C)
2000 Elsevier Science B.V. All rights reserved.
173. S. Sugita, T. Watanabe,
and A. Matsuda
"Atomic
image of a CuO2 plane in the STM image of a Bi2Sr2CaCu2O8+delta cleaved
surface"
Phys.
Rev. B 62 (13), 8715-8718 (2000).
ABSTRACT:
Clear atomic images of a Bi2Sr2CaCu2O8+delta (BSCCO) cleaved surface were
obtained at room temperature by scanning tunneling microscopy (STM). The
features of some observed images vary between two extreme cases, that is, the
Bi-O plane image and the CuO2 plane image. And we have succeeded in obtaining a
clear STM image of a CuO2 plane. From the CuO2 plane image, we found that this
plane had two superstructures, one along the a axis and the other along the b
axis. The periodicity of the superstructure along the b axis is (4-5)b, the
same as that in the Bi-O plane, and the periodicity along the a axis is 2a. To
explain these superstructures, we propose a lattice distortion model for the
CuO2 plane of BSCCO.
174. K. Sumitomo, H. Hibino, Y.
Homma, and T. Ogino
"Observation
of incomplete surface melting of Si using medium-energy ion scattering
spectroscopy"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 39
(7B), 4421-4424 (2000).
ABSTRACT: The
disordering of Si(lll) and Si(001) surfaces at high temperatures was
investigated using medium-energy ion scattering (MEIS). We clearly observed an
increase of MEIS scattering yield on channeling geometry at 1470 K for (111)
surface and at 1520 K for (001) surface. These results support the formation of
a liquid-like layer at the transition. We also found that there is a distinct
difference in the mode of disordering on Si(lll) and Si(001) surfaces. The
number of disordered atoms increases suddenly at the transition and remains
constant above the transition on Si(lll) surface. This picture of the
disordering is quite similar to the incomplete surface melting of Ge(lll)
surface. On the other hand, the thickness of disordered layer on Si(001) surface
continuously increases with temperature.
175. K. Sumitomo, K. Shiraishi,
Y. Kobayashi, T. Ito, and T. Ogino
"Surface
segregation and interdiffusion of Ge on Si(001) studied by medium-energy ion
scattering"
Thin
Solid Films 369 (1-2), 112-115 (2000).
ABSTRACT: The
mechanism of the surface segregation and interdiffusion of Ge on Si(001) during
epitaxial growth and annealing was studied using medium-energy ion scattering
(MEIS). One monolayer of Ge was grown on Si(001) at 450 degrees C and annealed
at 780 degrees C. The Ge was found to redistribute during the very early stages
(within 1 min) of the annealing process and remained constant even after
annealing at longer periods of time. Therefore, we conclude that the top few
layers attain thermal equilibrium in a short period of time, such as less than
1 min. The coverage dependence of Ge distribution in the top few layers was
also observed clearly from the surface of Ge deposited on Si(001) at 780
degrees C. This study strongly suggests that the subsurface phenomena should be
considered in order to more accurately describe the Si/Ge interface structure.
(C) 2000 Elsevier Science S.A. All rights reserved.
176. N. Susa
"Change
in transmittance due to free carriers in two-dimensional photonic
crystals"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 39
(11), 6288-6289 (2000).
ABSTRACT:
Numerical simulation revealed that photonic crystals consisting of dielectric
and air cylinders should have a high contrast at moderate optical power
densities (P) (less than 2 kW/cm(2)) when the number of stacked layers (ST,
i.e, thickness) is larger than or equal to 32. The peak wavelength shifted by
about -32 to -39 nm when P was increased from 0 to 10 kW/cm(2) at ST greater
than or equal to 32 The peak wavelength shifted more with P with a Smaller ST
because the peak wavelength at P = O became longer for the wavelengths
examined.
177. N. Susa
"Transmittance
for a two-dimensional photonic-crystal structure consisting of cylinders and
liquid crystal"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 39
(6A), 3466-3467 (2000).
ABSTRACT: The
transmittance for a two-dimensional photonic-crystal structure consisting of 8
x 8 cylinders filled with or surrounded by a liquid crystal was numerically
calculated using the scattering matrix method. When the refractive index of the
liquid crystal was increased from 1.4 to 1.6, the transmittance for the
liquid-crystal-filled cylinders increased from 4.5 x 10(-3) to 1 at a
wavelength of 825 nm, and that for the cylinders surrounded by the liquid
crystal increased from 1.3 x 10(-3) to 1 at 1060 nm (triangular lattice) and
from 3.0 x 10(-4) to 1 at 1140 nm (square lattice).
178. H. Suzuki
"Self-enhancement
in the electroluminescence of a near-infrared ionic dye"
Appl.
Phys. Lett. 76 (12), 1543-1545 (2000).
ABSTRACT:
This letter reports self-enhancement behavior observed in the near-infrared
electroluminescence (EL) of an ionic dye,
2-[6-(4-dimethylaminophenyl)-2,4-neopentylene-1,3,5-hexatrienyl]-3-methy
lbenzothiazolium perchlorate doped in poly(N-vinylcarbazole). The EL intensity
measured under a constant current, and therefore, the external EL quantum
efficiency (phi(ex)), increases with time both when the EL is generated
continuously in a constant current mode and kept in a no-bias field, whereas it
decreases in a reverse-bias field. With an enhancement factor of about 80 under
a constant current of 0.1 mA/cm2, phi(ex) reaches the 1% photons/electron
level. I conclude that the behavior originates from the enhanced electron and
hole injection caused by the alignment of the doped ionic dye molecules along
the bias field. (C) 2000 American Institute of Physics.
[S0003-6951(00)01612-0].
179. H. Suzuki, S. Hoshino, K.
Furukawa, K. Ebata, C. H. Yuan, and I. Bleyl
"Polysilane
light-emitting diodes"
Polym.
Adv. Technol. 11 (8-12), 460-467 (2000).
ABSTRACT:
This paper discusses the material factors which have led to a recent
breakthrough in polysilane light-emitting diodes (LEDs) made from a diaryl
polysilane, poly[bis(p-n-butylphenyl)silane] (PBPS), by comparing them with
LEDs which employ a conventional polysilane, poly(methylphenylsilane). In
contrast to LEDs based on conventional polysilanes in which a weak ultraviolet
Electroluminescence (EL) plas detected either with a strong broad visible EL or
only at low temperatures, room-temperature pure near-ultraviolet EL was
observed with a quantum? effciency of 0.1% photons/electron with an electron
injecting Al electrode in PBPS-LEDs. We examined the spectroscopic, electronic
and structural properties of PBPS, and ascribed to them the improvements
observed in the EL characteristics. We also mention the possible future
direction of polysilane LED research and other potential optoelectronics
applications of polysilanes to the active medium of lasers. Copyright (C) 2000
John Wiley & Sons, Ltd.
180. M. Suzuki and T. Watanabe
"Discriminating
the superconducting gap from the pseudogap in Bi2Sr2CaCu2O8+delta by interlayer
tunneling spectroscopy"
Phys.
Rev. Lett. 85 (22), 4787-4790 (2000).
ABSTRACT:
Tunneling spectroscopy using a very thin stack of intrinsic Josephson junctions
has revealed that the superconducting gap is definitely different from the
pseudogap in the Bi2Sr2CaCu2O8+delta system. In the underdoped region, the
conductance peak arising from the superconducting gap is independently observed
in the dI/dV-V curve and its position is much lower than that of the pseudogap.
Near the optimum doping level and in the overdoped region, both peaks are
located in close proximity. These findings are in conflict with a previous understanding
of the pseudogap.
181. S. Suzuki, C. Bower, Y.
Watanabe, and O. Zhou
"Work
functions and valence band states of pristine and Cs-intercalated single-walled
carbon nanotube bundles"
Appl.
Phys. Lett. 76 (26), 4007-4009 (2000).
ABSTRACT: The
electronic structures and the work functions of pristine and Cs-intercalated
single-walled carbon nanotube bundles were investigated using ultraviolet
photoemission spectroscopy. The valence bands of the pristine bundles were
considerably altered from those of graphite. A spectral shift to the higher
binding energy side was observed in the Cs-intercalated sample. The work
function of the pristine bundles was found to be 4.8 eV, which is 0.1-0.2 eV
larger than that of graphite. A drastic decrease of the work function to about
2.4 eV was observed in the Cs-intercalated sample. (C) 2000 American Institute
of Physics. [S0003-6951(00)05326-2].
182. S. Suzuki, T. Kiyokura, F.
Maeda, K. G. Nath, Y. Watanabe, T. Saitoh, and A. Kakizaki
"Resonant
photoemission spectroscopy of Ga 3d two-hole states of GaAs"
J.
Phys. Soc. Jpn. 69 (6), 1807-1811 (2000).
ABSTRACT: The
Ga 3d two-hole states were observed from GaAs(001)-c(4 x 4), -2 x 4, and
(110)-1 x 1 surfaces using resonant photoemission spectroscopy. Multiplet terms
(1)G, D-1, and F-3 were clearly distinguished at the photon energy around the
3(p) absorption threshold. The surface components of the two-hole states were
observed in the spectra of the (001)-2 x 4 and (110)-1 x 1 surfaces having Ga
atoms at the surfaces. The curve-fitting analysis revealed that the intensities
of the surface component of the two-hole states were considerably smaller than
those of the d(9) states. This is ascribed to the reduced absorption
probabilities of the 3p electrons at the surfaces caused by the surface
relaxation.
183. A. Taguchi and Y. Hirayama
"Stable
site and stable charge state of a fluorine atom in Si"
Solid
State Commun. 116 (11), 595-597 (2000).
ABSTRACT: We
investigated a stable state of a fluorine (F) atom in Si bulk by using
first-principles calculations. We considered Various interstitial sites and
three charge states from +1 to -1. We found that over a wide range of Fermi
levels, the bond center site in the +1 charge state is the most stable for an F
atom. The present calculations suggest that the experimentally observed
conductivity-dependent etching properties of F for Si are intimately related to
the charge-state-dependent stable site of F in the Si bulk. (C) 2000 Elsevier
Science Ltd. All rights reserved.
184. A. Taguchi, T. Ohno, and
T. Sasaki
"Fluorine
atoms in AlAs, GaAs, and InAs: Stable state, diffusion, and carrier
passivation"
Phys.
Rev. B 62 (3), 1821-1827 (2000).
ABSTRACT: We
investigated various basic properties of fluorine (F) atoms in AlAs, GaAs, and
InAs by using first-principles calculations. In these three semiconductors, we
found that the -1 charge state is the most stable in a wide range of Fermi
levels and that the F atom prefers sites surrounded by group-III atoms. These
characteristics can be understood by considering that F has the largest
electronegativity among the elements. We found that the diffusion properties,
such as the diffusion path and the diffusion barrier height, are similar in
these semiconductors. The estimated barrier heights are also comparable to the
experimentally obtained barrier height in Al(0.48)In(0.52)AS, suggesting that
the diffusion properties in AlxIn1-xAs are also similar. This implies that the
experimentally observed selective F incorporation into AlxIn1-xAs is not due to
the diffusion properties. It has been thought that the F atom forms a F-Si
defect complex in AlxIn1-xAs, but we found that a F atom in the -1 charge state
has stability comparable to that of a F-Si defect complex in binary
semiconductors, suggesting that F-Si defect complexes and isolated F atoms in
the -1 charge state coexist in AlxIn1-xAs. This coexistence is consistent with
the observation of the F-Si defect complex, as well as observed F doping
effects such as donor passivation and the decrease in the electron mobility.
Based on the present calculations for the binary semiconductors, some
characteristic properties of F in AlxIn1-xAs can be understood.
185. A. Taguchi, K. Shiraishi,
and T. Ito
"Stable
microstructures on a GaAs(111)A surface: The smallest unit for epitaxial
growth"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 39
(7B), 4270-4274 (2000).
ABSTRACT: We
investigated the stability of various microstructures constructed by several Ga
and As adatoms on a GaAs(111)A surface by using first-principles calculations.
We estimated the formation energies of the structures as a function of the
chemical potential and found a very stable structure composed of one Ga adatom
and three As adatoms. Investigations of the elemental growth process imply that
this structure is the smallest unit able to initiate epitaxial growth on the
GaAs(111)A surface. Based on the calculation results, we propose a growth
mechanism for the (111)A surface, which is characterized by the formation of a
stable structure and the subsequent coalescence of the structure. This
mechanism qualitatively explains the observed differences in the properties of
the growth islands on (111)A and (001) surfaces.
186. A. Taguchi, K. Shiraishi,
and T. Ito
"Self-surfactant
effect of As on a GaAs(111)A surface"
Appl.
Surf. Sci. 162, 354-358 (2000).
ABSTRACT: We
have theoretically investigated the effects of Ga- and As-adatom adsorption on
a GaAs(111)A surface to reveal the epitaxial growth mechanism by using
first-principles calculations. We found that the formation of Ga-Ga and Ga-As
coupled structures make the Ga-vacancy site stable, while our previous study
showed that the site is not the most stable site for one Ga-adatom adsorption.
We also found that the Ga-As coupled structure is more stable than the Ga-Ga
coupled structure, clearly indicating that As has a stronger stabilization
effect on the Ga-vacancy site for a Ga atom. The GaAs lattice is maintained by
the As adsorption in a self-organizing manner. Accordingly, As acts as a
self-surfactant element. The importance of As suggested by the present
calculations is consistent with the experimentally known fact that rather high As
pressure is needed for the growth of the GaAs epitaxial layers on a GaAs(111)A
surface. (C) 2000 Elsevier Science B.V. All rights reserved.
187. A. Taguchi, K. Shiraishi,
and T. Ito
"First-principles
study of the elemental process of epitaxial growth on a GaAs(111)A
surface"
Phys.
Rev. B 61 (19), 12670-12673 (2000).
ABSTRACT: We
theoretically investigated the elemental process of epitaxial growth on a
GaAs(111)A surface by using first-principles calculations. We estimated the
formation energies of various microstructures as a function of the chemical
potential, and found a very stable microstructure formed by a single Ga and
three As adatoms. This structure may be the smallest unit for the epitaxial
growth. The formation of such a stable microstructure is crucial for
stimulating the growth process. The need for such a stable microstructure
characterizes the growth mechanism for a GaAs(111)A surface, and results in the
different properties of the growth island between the GaAs(111)A and GaAs(001)
surfaces.
188. T. Takagahara
"Theory
of exciton doublet structures and polarization relaxation in single quantum
dots"
Phys.
Rev. B 62 (24), 16840-16855 (2000).
ABSTRACT: The
mechanism of exciton doublet structures in quantum dots is identified as the
long-range part of the electron-hole exchange interaction which is emphasized
by the anisotropic shape of quantum dots. The physical origin of the energetic
order of the orthogonally polarized exciton states of each doublet is clarified
by inspecting the spatial distribution of the exciton polarization. The key
concepts to understand the energetic order are the node configuration of the
distribution function of exciton polarization and the dipole-dipole interaction
energy originating from the long-range electron-hole exchange interaction. The
population relaxation and the polarization relaxation of excitons are studied
and the extremely slow polarization relaxation within exciton doublet states is
predicted. It is also found that the inter-doublet cross-relaxation between
orthogonally polarized exciton states occurs as efficiently as the population
relaxation.
189. T. Takagahara
"Theory
of exciton fine structures and extremely slow spin relaxation in single quantum
dots"
J.
Lumines. 87-9, 308-311 (2000).
ABSTRACT: A
comprehensive theory is proposed to describe the polarization-dependent fine
splitting of exciton doublet lines and the relation between the polarization
direction and the energy level order of doublet states in anisotropic quantum
dots. The extremely slow spin relaxation within exciton doublet states is
predicted. At the same time, it is found that the cross-relaxation between
orthogonally polarized exciton states is significant. (C) 2000 Elsevier Science
B.V. All rights reserved.
190. Y. Takahashi
"Single-electron
device - An ultimate device that operates on just a single electron"
Ntt
Rev. 12 (1), 12-16 (2000).
ABSTRACT: As
we approach a new age in which the amount of information communication is
expected to increase explosively, energy-saving in communication processing has
become an urgent issue. The single-electron device is the ultimate
low-power-consumption device because, as the name implies, it operates on just
a single electron. This article describes the operation mechanism of such
devices and new fabrication method for single-electron devices developed by NTT
Basic Research Laboratories. It also overviews new promising functions of such
devices.
191. Y. Takahashi, A. Fujiwara,
K. Yamazaki, H. Namatsu, K. Kurihara, and K. Murase
"Multigate
single-electron transistors and their application to an exclusive-OR gate"
Appl.
Phys. Lett. 76 (5), 637-639 (2000).
ABSTRACT: The
two-input exclusive-OR (XOR) function was implemented by a multigate
single-electron transistor (SET). Two types of multigate SETs operating at 40 K
were fabricated on a top silicon layer of an Si-on-insulator wafer by using a
special technique called pattern-dependent oxidation. Two small gate electrodes
which act as the input gates were formed over the small SET island. The output
current of the devices took a high level when a high voltage was applied to
either of the two gates with the other gate grounded, while it took a low level
when both gates were grounded or fed with a high voltage. It is striking that
such an XOR function can be implemented with just one device. (C) 2000 American
Institute of Physics. [S0003-6951(00)02005-2].
192. H. Takayanagi, H. Ando,
and T. Fujisawa
"From
quantum effects to quantum circuits - Toward the quantum computer"
Ntt
Rev. 12 (1), 17-25 (2000).
ABSTRACT: The
quantum computer is designed to harness the unique uncertainties of quantum
mechanics at the micro level to enable ultra-rapid calculations at hitherto
unimaginable speeds. In this article, we describe the progress of research from
the quantum effect to quantum gate circuits and the quantum computer, citing
three research fields at the NTT Basic Research Laboratories - quantum dot
molecules, optical quantum dots and superconducting loops.
193. H. Tamura, K. Shiraishi,
and H. Takayanagi
"Ferromagnetism
in semiconductor dot array"
Jpn.
J. Appl. Phys. Part 2 - Lett. 39 (3AB), L241-L243 (2000).
ABSTRACT: Ferromagnetism
in semiconductor-dot arrays is theoretically predicted. The two types of
bipartite semiconductor-dot arrays which we propose exhibit flat band
characteristics. According to the Lieb theorem, ferromagnetism is predicted,
although our designed dot arrays do not contain any magnetic elements. We also
investigate the typical dot-radius and inter-dot distance for the realization
of the semiconductor-dot ferromagnetism, and several applications are
discussed.
194. S. Tarucha, D. G. Austing,
S. Sasaki, Y. Tokura, W. van der Wiel, and L. P. Kouwenhoven
"Effects
of Coulomb interactions on spin states in vertical semiconductor quantum
dots"
Appl.
Phys. A-Mater. Sci. Process. 71 (4), 367-378 (2000).
ABSTRACT: The
effects of direct Coulomb and exchange interactions on spin states are studied
for quantum dots contained in circular and rectangular mesas. For a circular
mesa a spin-triplet favored by these interactions is observed at zero and
nonzero magnetic fields. We tune and measure the relative strengths of these
interactions as a function of the number of confined electrons. We find that
electrons tend to have parallel spins when they occupy nearly degenerate
single-particle states. We use a magnetic field to adjust the single-particle
state degeneracy, and find that the spin-configurations in an arbitrary
magnetic field are well explained in terms of two-electron singlet and triplet
states. For a rectangular mesa we observe no signatures of the spin-triplet at
zero magnetic field. Due to the anisotropy in the lateral confinement
single-particle state degeneracy present in the circular mesa is lifted, and
Coulomb interactions become weak. We evaluate the degree of the anisotropy by
measuring the magnetic field dependence of the energy spectrum for the ground
and excited states, and find that at zero magnetic field the spin-singlet is
more significantly favored by the lifting of level degeneracy than by the
reduction in the Coulomb interaction. We also find that the spin-triplet is
recovered by adjusting the level degeneracy with magnetic field.
195. S. Tarucha, D. G. Austing,
Y. Tokura, W. G. van der Wiel, and L. P. Kouwenhoven
"Direct
Coulomb and exchange interaction in artificial atoms"
Phys.
Rev. Lett. 84 (11), 2485-2488 (2000).
ABSTRACT: We
determine contributions from the direct Coulomb and exchange interactions to
the total interaction in artificial semiconductor atoms. We tune the relative
strengths of the two interactions and measure them as a function of the number
of confined electrons. The electrons tend to have parallel spins when they
occupy nearly degenerate single-particle states. We use a magnetic field to
adjust the single-particle-state degeneracy, and find that the spin
configurations in an arbitrary magnetic field are well explained in terms of
two-electron singlet and triplet states.
196. G. Tatara and Y. Tokura
"Electronic
pressure on the ferromagnetic domain wall"
Solid
State Commun. 116 (10), 533-538 (2000).
ABSTRACT: The
scattering of electron by a domain wall in a nano-wire is studied
perturbatively to the lowest order. The correction to the thermodynamic
potential of the electron system due to scattering is calculated from the:
phase shift. The wall profile is determined by taking account of this
correction, and the result indicates that the wall in a ferromagnet with a
small exchange coupling can be squeezed to be very thin to lower the electron
energy. (C) 2000 Published by Elsevier Science Ltd.
197. T. Tateno and Y. Jimbo
"Stochastic
mode-locking for a noisy integrate-and-fire oscillator"
Phys.
Lett. A 271 (4), 227-236 (2000).
ABSTRACT: We
investigated the ways in which noise influences lower-order mode-locked regions
(Arnold tongues) in the parameter space of an integrate-and-fire model with a
periodically modulated threshold. To study the stochastic mode-locking in the
model, we use the first-passage-time problem of the Ornstein-Uhlenbeck process
with a periodic boundary to define the Markov operator governing the transition
of a threshold phase density. We present a numerical method for evaluating
stochastic bifurcation by spectral analysis of the operator and briefly discuss
the implications for biological systems. (C) 2000 Elsevier Science B.V. All
rights reserved.
198. Y. Tokura, S. Sasaki, D.
G. Austing, and S. Tarucha
"Single-electron
tunneling through two vertically coupled quantum dots"
Physica
E-Low-Dimensional Systems & Nanostructures 6
(1-4), 676-679 (2000).
ABSTRACT:
Electron states and tunneling properties of two vertically coupled quantum dots
are analyzed. The energy mismatch of the dots affects the phase diagram as a
function of the quantum mechanical coupling and magnetic field normal to the
plane. A magnetic field parallel to the barrier mixes the single particle
states and also induces a singlet-triplet transition. (C) 2000 Elsevier Science
B.V. All rights reserved.
199. E. Toyoda, H. Takayanagi,
and H. Nakano
"Gate-modified
giant Andreev backscattering in a superconductor-semiconductor junction"
J.
Phys. Soc. Jpn. 69 (6), 1801-1806 (2000).
ABSTRACT: We
investigated giant Andreev backscattering (GAB) in a superconductor
(S)-semiconductor two-dimensional electron gas (2DEG) junction with a special
gate configuration: a split gate which produces a quantum point contact (QPC)
and an ordinary wide gate set between S and the QPC, which alters the
properties of the diffusive transport in the 2DEG. Different combinations of
the two gates voltages offered us a many "samples" for one junction,
which enabled us to systematically study GAB. By applying a negative split gate
voltage, the number of modes in the QPC was decreased and a crossover from the
reentrant conductance of the disordered 2DEG to enhanced (peaked) QPC
conductance was observed. The peak width at different degrees of diffusiveness
clearly showed that coherent Andreev backscattering is essential for the
enhancement. We discuss the influence of the bias voltage and the magnetic
field on the enhancement quantitatively.
200. E. Toyoda, H. Takayanagi,
and H. Nakano
"Gate-modified
giant Andreev backscattering"
Physica
B 284, 569-570 (2000).
ABSTRACT: We
investigated giant Andreev backscattering in a superconductor (S) - two-dimensional
electron gas (2DEG) junction with two kinds of gate: a quantum point contact
(QPC) and an ordinary wide gate. Though the diffusive 2DEG itself displayed
reentrant conductance, by attaching a QPC we observed conductance enhancement
(peak) at zero energy. The bias voltage and the magnetic field dependence of
the enhancement at different degrees of dirtiness showed that phase conjugation
between an electron and a hole is essential for enhancement. (C) 2000 Elsevier
Science B.V. All rights reserved.
201. S. Toyoda, M. Fujiki, C.
H. Yuan, and R. West
"Ionochromism
and increase in fluorescence quantum yield of an ether-substituted polysilylene
upon adding lithium ions in solution"
Macromolecules 33
(5), 1503-1504 (2000).
ABSTRACT:
202. M. Uematsu
"Diffusion
simulation of ultra-low-energy implanted boron in silicon"
Jpn.
J. Appl. Phys. Part 2 - Lett. 39 (9AB), L895-L897 (2000).
ABSTRACT:
dfWe have simulated the diffusion of boron (B) after ultra-low-energy
implantation in silicon during post-implantation annealing, based on our model
[M. Uematsu: Jpn. J. Appl. Phys. 38 (1999) 3433]. When the B concentration is
not so high (less than or similar to 1 x 10(21) cm(-3)), the experimental B
depth profiles are fitted using the model with taking into account B
segregation to silicon oxide at the surface. When the B concentration is very
high (greater than or similar to 1 x 10(21) cm(-3)), however, the simulation
underestimates the diffusion, which is attributable to boron-enhanced
diffusion. The self-interstitial emission from a silicon boride layer in the
high B concentration region is taken into account, and the simulation well
reproduces the experimental profiles.
203. M. Uematsu
"Simulation
of boron diffusion in high-dose BF2 implanted silicon"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 39
(4A), 1608-1611 (2000).
ABSTRACT: We
have simulated the transient enhanced diffusion (TED) of boron (B) after
amorphizing BF2 ion implantation in silicon. A unified simulation is done based
on the models for B diffusion, for TED by self-interstitial clusters, for B
clustering and B precipitation, and for end-of-range (EOR) defects. The
simulation overestimates the diffusion using the normal values for the
efficiency of EOR defects as a source of self-interstitials. The simulation
well reproduces the experimental profiles when the efficiency is reduced so
that the defects maintain self-interstitial concentration at thermal
equilibrium values. This reduction is attributable to the presence of fluorine
at EOR defect sites, which may prevent the release of self-interstitials, In
addition, the second peak near the amorphous/crystalline (a/c) interface
observed in experimental profiles is reproduced, and the peak is attributed to
B precipitates.
204. M. Uematsu
"Transient
enhanced diffusion and deactivation of high-dose implanted arsenic in silicon"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 39
(3A), 1006-1012 (2000).
ABSTRACT: We
have simulated the transient enhanced diffusion (TED) of high-concentration
arsenic (As) in silicon during postimplantation annealing. A unified simulation
was done, based on models for As diffusion, for TED by self-interstitial
clusters, and for end-of-range (EOR) defects. We have taken into account As
complex formation and As precipitation, which cause the As deactivation. We
have satisfactorily fitted As depth profiles at high doses (1-5 x 10(15)
cm(-2)) in a wide range of annealing conditions (750-1000 degrees C). The As
complex formation plays an important role in determining the diffusion profiles
through the self-interstitial emission upon the formation at lower temperatures
and through As deactivation at higher temperatures. The simulation results
suggest that boron (B) segregation toward the As tail regions is associated
with self-interstitial distributions determined by EOR defects and As profiles.
205. M. Uematsu, H. Kageshima,
and K. Shiraishi
"Oxidation
simulation of (111) and (100) silicon substrates based on the interfacial
silicon emission model"
Jpn.
J. Appl. Phys. Part 2 - Lett. 39 (11B), L1135-L1137 (2000).
ABSTRACT:
Silicon oxidation of(111) and (100) substrates is simulated based on the
interfacial silicon emission model. Large silicon emission from the interface,
which governs the oxidation rate at the interface, plays an important role in
determining the substrate-orientation dependence. The simulation is done by
changing only the rate of Si-atom emission from the interface. the emission
rate for (111) is about 0.4 times that for (100). Using a unified set of
parameters, the whole range of oxide thickness is fitted in a wide range of
oxidation temperatures (800-1200 degreesC) and oxygen pressures (1-20 atm).
206. M. Uematsu, H. Kageshima,
and K. Shiraishi
"Simulation
of high-pressure oxidation of silicon based on the interfacial silicon emission
model"
Jpn.
J. Appl. Phys. Part 2 - Lett. 39 (10A), L952-L954 (2000).
ABSTRACT:
Silicon oxidation using high-pressure oxygen, where the rate shows
less-than-linear dependence, is simulated based on the interfacial silicon
emission model. The oxidation reaction of the emitted Si atoms in the oxide,
which controls the oxidation rare at the interface, plays an important role in
determining the oxidation pressure dependence. We introduce reaction terms for
the oxidation in the oxide so as to fit the oxide thickness at oxygen pressures
of 1-20 arm. The simulation is made using constant parameter values for
oxidation reaction by changing only the oxidant solubility in the oxide in
proportion to oxygen pressure.
207. M. Uematsu, H. Kageshima,
and K. Shiraishi
"Unified
simulation of silicon oxidation based on the interfacial silicon emission
model"
Jpn.
J. Appl. Phys. Part 2 - Lett. 39 (7B), L699-L702 (2000).
ABSTRACT: We
have simulated silicon oxidation taking into account the emission of a large
number of silicon atoms from the interface, which governs the silicon-oxidation
rate. The silicon emission model enables the simulation to be done using the
oxidant self-diffusivity in the oxide with a single activation energy. The
simulation has deduced a silicon emission rate that exhibits a break point in
its activation energy at around 1000 degrees C, which is attributed to the
viscoelastic properties of the oxide, Using a unified set of parameters, the
whole range of oxide thickness is fitted in a wide range of oxidation
temperatures (800-1200 degrees C) without any empirical modifications.
208. W. G. van der Wiel, S. De
Franceschi, T. Fujisawa, J. M. Elzerman, S. Tarucha, and L. P. Kouwenhoven
"The
Kondo effect in the unitary limit"
Science 289
(5487), 2105-2108 (2000).
ABSTRACT: We
observe a strong Kondo effect in a semiconductor quantum dot when a small
magnetic field is applied. The Coulomb blockade for electron tunneling is
overcome completely by the Kondo effect, and the conductance reaches the
unitary Limit value. We compare the experimental Kondo temperature with the
theoretical predictions for the spin-1/2 Anderson impurity model. Excellent
agreement is found throughout the Kondo regime. Phase coherence is preserved
when a Kondo quantum dot is included in one of the arms of an Aharonov-Bohm
ring structure, and the phase behavior differs from previous results on a
non-Kondo dot.
209. T. Watanabe, T. Fujii, and
A. Matsuda
"Pseudogap
in Bi2Sr2CaCu2O8+delta studied by measuring anisotropic susceptibilities and
out-of-plane transport"
Physica
C 341, 931-932 (2000).
ABSTRACT: We
find in the Bi2Sr2CaCu2O8+delta system that the characteristic temperatures
T-chi* (below which the uniform susceptibilities chi (ab)(T) (H perpendicular
to c) and chi (c)(T) (H // c) decrease) and T-rhoc* (below which the
out-of-plane resistivity rho (c)(T) shows typical upturn) coincide for all
doping levels. We attribute the T dependence of chi 's and rho (c) to the
anomalous (pseudogapped) density-of-states (DOS) in high-T-c cuprates. In
addition, an analysis of the anisotropy in the T dependence of chi 's shows
that the high-temperature component (d chi /dT < 0) is also caused by a DOS
effect.
210. T. Watanabe, T. Fujii, and
A. Matsuda
"Pseudogap
in Bi2Sr2CaCu2O8+delta studied by measuring anisotropic susceptibilities and
out-of-plane transport"
Phys.
Rev. Lett. 84 (25), 5848-5851 (2000).
ABSTRACT:
find in the Bi2Sr2CaCu2O8+delta system that the characteristic temperatures
T-chi* [below which the uniform susceptibilities chi(ab)(T) (H perpendicular to
c) and chi(c)(T) (H parallel to c) decrease] and T-rho c* [below which the
out-of-plane resistivity rho(c)(T) shows typical upturn] coincide for all
doping levels. We attribute the T dependence of chi's and rho(c), to the
anomalous (pseudogapped) density of states (DOS) in high-T-c cuprates,
Furthermore, the anisotropy in the T dependence of chi's is universal, i.e.,
chi, proportional to 1.6 chi(ab), showing that there is only a single
T-dependent component in the chi's. This implies that the Curie-like behavior
(d chi/dT < 0) observed in overdoped samples is also caused by a DOS effect.
211. Y. Watanabe and F. Maeda
"Effect
of strain on the chemical bonds in InAs nanocrystals self-organized on GaAs and
Se-terminated GaAs surfaces"
Appl.
Surf. Sci. 162, 625-629 (2000).
ABSTRACT: We
employed surface sensitive photoelectron spectroscopy (PES) using synchrotron
radiation to investigate the strain of both deposited InAs and GaAs substrates
with and without Se-termination. The two distinct chemical components
comprising Ga-As bonding and In-As bonding states in the As 3d spectrum are
clearly observed for the first time, which indicates that the strain in both
the deposited InAs and GaAs substrates can be separately evaluated using the
core-level energy difference between the respective core-level chemical
components. This difference between the chemical components of Ga 3d and As 3d
levels for both two kinds of samples is found to be independent of InAs
deposition time, and to be almost the same as that of a bulk GaAs, implying
that no strain is generated in both two type GaAs substrates. On the other
hand, in the case of the deposited InAs, this value increases with an increase
in the layer thickness of InAs for the InAs/GaAs system and approaches to a
bulk InAs value, whereas, there exits only a slight change for the InAs/Se/GaAs
system at the very early stages of InAs growth and is almost the same as a bulk
InAs value. These results suggest that the driving force for the formation of
InAs nanocrystals in the InAs/GaAs system is the elastic strain, whereas, in
the InAs/Se/GaAs system, passivation-induced self-organizing mechanism is
crucial. (C) 2000 Elsevier Science B.V. All rights reserved.
212. H. Yamamoto, M. Naito, and
H. Sato
"A
new superconducting barium cuprate prepared by molecular beam epitaxy"
Physica
C 338 (1-2), 29-37 (2000).
ABSTRACT:
This paper reviews the MBE-synthesis and structural characterization of a new
superconducting barium cuprate Ba2CuO4-delta (Te less than or equal to 90 K).
The keys to the successful synthesis of this superconductor are (1) the
preparation of Ba2CuO3 in a CO2/H2O-free environment and (2) structural
transformation from insulating Ba2CuO3 with 1D CuO chains to superconducting
Ba2CuO4-delta with 2D CuO2 planes by strong ozone oxidation after growth. The
merits of MBE as a potential synthetic route in the search for new cuprate
superconductors are also discussed. (C) 2000 Elsevier Science B.V. All rights
reserved.
213. Y. Yamamoto
"Semiconductor
physics - Half-matter, half-light amplifier"
Nature 405
(6787), 629-630 (2000).
ABSTRACT:
214. M. Yamashita, M. Koashi,
T. Mukai, M. Mitsunaga, and N. Imoto
"Dynamics
of evaporative cooling in magnetically trapped atomic hydrogen"
Phys.
Rev. A 62 (3), art. no.-033602 (2000).
ABSTRACT: We
study the evaporative cooling of magnetically trapped atomic hydrogen on the
basis of the kinetic theory of a Bose gas. The dynamics of trapped atoms is
described by the coupled differential equations, considering both the
evaporation and dipolar spin relaxation processes. The numerical time-evolution
calculations quantitatively agree with the recent experiment of Bose-Einstein
condensation with atomic hydrogen. It is demonstrated that the balance between
evaporative cooling and heating due to dipolar relaxation limits the number of
condensates to 9X10(8) and the corresponding condensate fraction to a small
value of 4% as observed experimentally.
215. H. Yoshikawa, Y. Andoh, M.
Yamamoto, K. Fukuzawa, T. Tamamura, and T. Ohkubo
"7.5-MHz
data-transfer rate with a planar aperture mounted upon a near-field optical
slider"
Opt.
Lett. 25 (1), 67-69 (2000).
ABSTRACT: We
fabricated a planar aperture-mounted (PAM) slider by use of a focused ion beam
to demonstrate fast data acquisition for near-field optical data storage. The
aperture (200 nm X 500 nm) was formed upon the Ti-coated air-bearing surface of
the slider and was directly illuminated with a laser (lambda = 532 nm) beam
spot by use of an objective lens (N.A., 0.55). The light transmitted through
the aperture was modulated by a Ti-coated SiO2 disk with 200- and 400-nm-wide
line-and-space (L&S) patterns engraved by electron-beam lithography. The
optical throughput of the taperless aperture was greater than 0.02. By use of
the PAM slider, 400- and 200-nm L&S signals were detected at linear
velocities of 6 and 3 m/s, respectively, corresponding to a data-transfer rate
of 7.5 MHz. (C) 2000 Optical Society of America.
216. J. D. Yu, M. Natsuisaka,
H. Kato, S. Matsumoto, K. Kinoshita, T. Itami, and S. Yoda
"Studies
on molten glass sealing in diffusion coefficient measurements using shear cell
technique"
Rev.
Sci. Instrum. 71 (5), 2111-2116 (2000).
ABSTRACT: To
develop a shear cell technique for measuring the diffusion coefficient of
molten materials with high vapor pressure, molten silica glass was used to seal
the vapor leak from the clearance between the cell and the rotating rod. An
apparatus was designed to investigate the sealing ability of several molten
silica glasses. Using Corning 0211, 7059, and 7740 silica glasses, Ar could be
sealed under 150 kPa in the 1100-1500 K temperature range. The corresponding
viscosities of the molten silica glasses in the sealing temperature range were
10(5.3)-10(3.8) Pa s. Based on the results of Ar sealing experiments, the
configuration of molten glass sealing was used to seal the As vapor leak in
InxGa1-xAs diffusion coefficient measurement experiments. The As vapor leak was
successfully sealed and excellent diffusion coefficient measurement data were
obtained using the shear cell technique during microgravity experiments carried
out on sounding rocket. (C) 2000 American Institute of Physics.
[S0034-6748(00)04505-6].