1992 (with abstract) |
|
▼ Ordered by first author |
1. J.
Akimitsu, M. Uehara, M. Ogawa, H. Nakata, K. Tomimoto, Y. Miyazaki, H. Yamane,
T. Hirai, K. Kinoshita, and Y. Matsui
"Superconductivity
In The New Compound (Y1-Xcax)0.95sr2.05cu2.4(Co3)0.6oy"
Physica
C 201 (3-4), 320-324 (1992).
ABSTRACT: A
new Cu-oxide superconductor (Y1-xCax)0.95Sr2.05Cu2.4(CO3)0.6Oy has been found
by resistivity and magnetization measurements. The transition temperature is
about 63 K. The crystal structure consists of the periodic replacements of the
Cu(I) site with a CO3 group in the basic YBa2Cu3Oy structure.
2. H.
Asahi, S. J. Yu, J. Takizawa, S. G. Kim, Y. Okuno, T. Kaneko, S. Emura, S.
Gonda, H. Kubo, C. Hamaguchi, and Y. Hirayama
"Ingaasp/Inp
Quantum Wires Fabricated By Focused Ga Ion-Beam Implantation"
Surf.
Sci. 267 (1-3), 232-235 (1992).
ABSTRACT:
InGaAsP/InP quantum-wire structures are fabricated by focused Ga ion beam
implantation onto InGaAs/InP single quantum well (QW) structures. It is found
that InGaAsP layers produced by the intermixing of InGaAs/InP QW's by Ga ion
implantation and subsequent thermal annealing are nearly lattice matched to the
InP substrate. Fabricated quantum-wire structures exhibit photoluminescence
spectra showing a large blue shift, which is induced by the carrier confinement
into wire structures and the change of well composition.
3. J.
L. Chern, K. Otsuka, and P. Mandel
"Effects
Induced By Transit-Time On A Coupled 2-Element Optical Bistable Device"
IEEE
J. Quantum Electron. 28 (2), 555-561 (1992).
ABSTRACT: In
this paper, we study the effects of finite transit time, i.e., delay, on
dynamics in a coupled two-element optical bistable device. Here finite transit
time is considered because of signal propagation between the elements. It is
shown that delay can be used as a measure of crosstalk between the coupled
elements and it will increase the "lethargy time." Thus, many
interesting, transient phenomena take place both in hysteresis and pitchfork
(symmetry-breaking) regimes. Symmetry-recovering crisis originating from the
collision between the unstable periodic orbit and chaotic asymmetrical solution
is predicated to occur for T almost-equal-to-tau (T: transit time, tau:
response time of nonlinear medium). It is shown that symmetry-recovering crisis
results in switching failure in set-reset (S-R) flip-flop operations with
pitchfork bifurcation structure.
4. R.
Cingolani, M. Lepore, R. Tommasi, I. M. Catalano, H. Lage, D. Heitmann, K.
Ploog, A. Shimizu, H. Sakaki, and T. Ogawa
"2-Photon
Absorption In Gaas Quantum Wires"
Phys.
Rev. Lett. 69 (8), 1276-1279 (1992).
ABSTRACT: We
have investigated the polarization-dependent two-photon absorption in
GaAs/AlGaAs quantum wires. The anisotropic selection rules of the multiphoton
absorption process are exploited to study the one-dimensional 2p exciton states
and the transitions between quantum wire subbands of different quantum numbers
(DELTA-n(y) not-equal 0 selection rule). The deviations from the selection
rules derived for the strict one-dimensional case are discussed, and depend on
the actual quasi-one-dimensional character of the excitonic wave functions.
5. K.
W. Delong and J. Yumoto
"Chirped
Light And Its Characterization Using The Cross-Correlation Technique"
J.
Opt. Soc. Am. B-Opt. Phys. 9 (9), 1593-1604 (1992).
ABSTRACT: We
analyze the Cross-correlation (SUM-frequency generation) method of chirp
measurement of short light pulses. We find that there are two complementary
methods to measure the chirp, depending on whether the pump has a larger
temporal or spectral resolution than the pulse to be measured. We show how to
relate these measurements of chirp to the time domain description for linear
chirp. We also discuss the use of this method in measuring nonlinear chirps. We
demonstrate experimentally the dependence of the results of the measurement on
the spectral response function of the monochromator.
6. S.
R. Friberg
"Optical
Solitons For Signal-Processing"
IEICE
Trans. Fundam. Electron. Commun. Comput. Sci. E75A
(1), 5-11 (1992).
ABSTRACT: We
consider applications of optical solitons to signal processing. Soliton
switching devices promise ultrafast operation and compatibility with
communications systems using optical pulses. Quantum soliton effects include
broadband squeezing and quantum nondemolition measurements, and can reduce
noise and increase sensitivities of optical measurements. We report the
demonstration of two-color soliton switching and describe progress towards
implementation of quantum nondemolition measurement of photon number using
soliton collisions.
7. S.
R. Friberg
"Optical
Solitons For Signal-Processing"
IEICE
Trans. Electron. E75C (1), 3-9 (1992).
ABSTRACT: We
consider applications of optical solitons to signal processing. Soliton
switching devices promise ultrafast operation and compatibility with
communications systems using optical pulses. Quantum soliton effects include
broadband squeezing and quantum nondemolition measurements, and can reduce
noise and increase sensitivities of optical measurements. We report the
demonstration of two-color soliton switching and describe progress towards
implementation of quantum nondemolition measurement of photon number using
soliton collisions.
8. S.
R. Friberg and K. W. Delong
"Breakup
Of Bound Higher-Order Solitons"
Opt.
Lett. 17 (14), 979-981 (1992).
ABSTRACT:
Bound higher-order solitons, sometimes called breather solitons, can easily be
broken apart by small perturbations. We discuss the conditions for breakup of
bound solitons and describe a method to determine the details of the soliton
breakup. Using this method, we illustrate the breakup of bound solitons by
optical filters, by asymmetric FM modulation (not AM or symmetric FM
modulation), and by superposition with other optical pulses.
9. S.
R. Friberg, S. Machida, and Y. Yamamoto
"Quantum-Nondemolition
Measurement Of The Photon Number Of An Optical Soliton"
Phys.
Rev. Lett. 69 (22), 3165-3168 (1992).
ABSTRACT: We
report the quantum-nondemolition measurement of the photon number of an optical
soliton. Taking advantage of the conservation properties of quantum solitons,
we were able to read out the photon number of a "signal" soliton via
the phase of a "probe" soliton after a soliton collision in a
single-mode low-loss optical fiber. Subsequent noise measurements showed the
photon number fluctuations of the signal soliton at the shot-noise limit to be
correlated to the phase fluctuations of the probe soliton, signifying a
backaction-evading measurement of the photon number.
10. M.
Fujiki
"Structural
Defects In Poly(Methylphenylsilylene)"
Chem.
Phys. Lett. 198 (1-2), 177-182 (1992).
ABSTRACT: The
Si-based structural defects in poly(methylphenylsilylene) backbones were
detected as two new Si-29 NMR signals and as two new Si-Si vibrational IR
bands. The defects, consisting of an organosilyne unit and about three
methylphenylsilylene monomer units near the branch, were presumed to be in a
fairly lengthened Si-Si bonding state. The empirical linear relationship
between the relative intensity of broad photoluminescence and the defect
density predicts the disappearance of the broad luminescence for a defect
density of less than 1 %.
11. M.
Fujino, T. Hisaki, M. Fujiki, and N. Matsumoto
"Preparation
And Characterization Of A Novel Organopolysilane -
(3,3,3-Trifluoropropyl)Methylpolysilane"
Macromolecules 25
(3), 1079-1083 (1992).
ABSTRACT: The
first soluble (fluoroalkyl)polysilane high polymer was prepared by a
conventional Wurtz-type reaction of dichlorosilane and sodium in n-paraffins
above 150-degrees-C. The structure of this polymer was determined by elemental
analyses (C and H), gel permeation chromatography, and spectral analyses
[FT-IR, FT-NMR (H-1, C-12, F-19, and Si-29), and UV]. The molecular weight
distribution of the polymer was monomodal, and the weight-average molecular
weight of this polymer was 31 000. The UV absorption maximum due to Si
catenation was at 285 nm. This is the shortest wavelength yet reported for an
organopolysilane high polymer. The thermochromic behavior of this polymer was
also observed in the solid state at temperatures from -120 to + 100-degrees-C.
The polymer began to decompose at around 200-degrees-C, and its glass
transition temperature was -3-degrees-C, which was higher than that of the
nonfluorinated polymer.
12. Y. K.
Fukai, S. Tarucha, Y. Hirayama, Y. Tokura, and T. Saku
"Reflection
And Refraction Of Ballistic Electrons Through Different Carrier Concentration
Regions"
Appl.
Phys. Lett. 60 (1), 106-108 (1992).
ABSTRACT:
Transmission and reflection characteristics of ballistic electrons are studied
in a macroscopic four-terminal square device with a strip Schottky gate placed
so as to bisect the device. Since the gate is negatively biased, a bend
resistance peak at zero magnetic field, which is induced by ballistic electron
injection into an opposite voltage probe, varies from positive to negative, and
a magnetic focusing peak shifts to a lower field. These phenomena arise from
the reflection of ballistic electrons crossing regions of different electron
densities. The transmission and reflection probabilities are determined as a
function of gate voltage, and are related to the change in the refractive index
of ballistic electrons.
13. T. Fukui
and S. Ando
"Gaas
Tetrahedral Quantum Dots Grown By Selective Area Mocvd"
Superlattices
Microstruct. 12 (2), 141-144 (1992).
ABSTRACT:
14. T.
Fukui, S. Ando, T. Honda, and T. Toriyama
"Gaas
Tetrahedral Quantum Dot Structures Fabricated Using Selective Area Mocvd"
Surf.
Sci. 267 (1-3), 236-240 (1992).
ABSTRACT: New
GaAs quantum dot structures, called tetrahedral quantum dots (TQD's), are
proposed to make a zero-dimensional electron-hole system. The TQD's are
surrounded by crystallographic facets fabricated using selective area MOCVD on
GaAs(111)B substrates. The calculated energy sublevel structures of
zero-dimensional electrons in a GaAs TQD show large quantum size effects,
because electrons are confined three-dimensionally. GaAs and AlGaAs tetrahedral
facet structures were grown using MOCVD on GaAs(111)B substrates partially
etched into a triangular shape. Tetrahedral growth with {110} facets occurs in
the triangular areas. The cathodoluminescence intensity map for GaAs
tetrahedrons buried in AlGaAs shows the tetrahedral dot array.
15. T.
Fukui, H. Saito, M. Kasu, and S. Ando
"Mocvd
Methods For Fabricating Gaas Quantum Wires And Quantum Dots"
J.
Cryst. Growth 124 (1-4), 493-496 (1992).
ABSTRACT:
Semiconductor low-dimensional structures such as quantum wires and quantum dots
fabricated by metalorganic chemical vapor deposition (MOCVD) are reported.
GaAs/AlAs quantum wire arrays including fractional-layer superlattices were
grown on (001) GaAs vicinal surfaces. Uniform lateral superlattices were
observed by transmission electron microscopy. However, polarization-dependent
photoluminescence and the optical absorption spectra suggest that significant
alloying occurs in AlAs/GaAs vertical interfaces. GaAs tetrahedral quantum dots
buried in AlGaAs were also fabricated on a SiO2 masked (111)B GaAs substrate
partially etched to a triangular shape. First, AlGaAs truncated tetrahedral
structures with three {110} facets were grown on GaAs triangular areas. Next,
GaAs dot structures were sequentially grown on top of the AlGaAs truncated
tetrahedron. Finally, AlGaAs was over-grown on {110} sidewall facets with a
different growth condition. We observed large quantum size effects for about
100 nm TQD in low temperature photoluminescence, which is in good agreement
with calculations.
16. T.
Fukui, K. Tsubaki, H. Saito, M. Kasu, and T. Honda
"Fractional
Superlattices Grown By Mocvd And Their Device Applications"
Surf.
Sci. 267 (1-3), 588-592 (1992).
ABSTRACT:
(AlAs)1/2(GaAs)1/2 fractional-layer superlattices (FLS's) are grown on (001)
vicinal substrates by metalorganic chemical vapor deposition. Various kinds of
GaAs substrates were used. When the substrate is misoriented to [110] by
1.92-degrees and [110] by 0.10-degrees, uniform superlattice periods over a
large surface area are observed by bright field transmission electron
microscopy (TEM). The results suggest the ideal growth from a kink site occurs
during MOCVD growth, and the distances between kink sites are equal. On a
substrate misoriented to [110] by 1.90-degrees, the superlattice periods
exhibit an undulation. This shows that kink flow mode growth is not dominant in
the [110] direction. On a substrate misoriented to [010] by 2.0-degrees, no
superlattice periods were observed. From the above results, we discuss the
growth mechanisms. Polarization dependent photoluminescence and optical
absorption spectra of FLS's were also observed. Electron wave interference
devices with lateral periodic potential were fabricated.
17. K.
Furukawa, M. Fujino, and N. Matsumoto
"Cubic
Silicon Cluster"
Appl.
Phys. Lett. 60 (22), 2744-2745 (1992).
ABSTRACT: A
cubic silicon cluster having eight bonds each terminated by a tert-butyl
substituent, tert-butyloctasilacubane (TBOSC), is studied. TBOSC was formed and
isolated by chemical procedures. The optical properties of TBOSC were measured
in comparison with those of bulk silicon. TBOSC is purple and its absorption
edge (lambda(g)) is observed at 650 nm (1.9 eV) at room temperature. This
lambda(g) is 0.8 eV larger than that of bulk silicon. It also shows
photoluminescence extending to 850 nm at 77 K although bulk silicon shows no
photoluminescence.
18. A.
Furusaki, H. Takayanagi, and M. Tsukada
"Josephson
Effect Of The Superconducting Quantum Point Contact"
Phys.
Rev. B 45 (18), 10563-10575 (1992).
ABSTRACT: The
dc Josephson effect of a constriction in a two-dimensional
superconductor-semiconductor-superconductor junction, i.e., a superconducting
quantum point contact, is investigated theoretically for both long and short
constriction lengths compared with the superconducting coherence length. It is
shown that the critical current of a ballistic superconducting quantum point
contact increases stepwise as a function of its width under appropriate
conditions. The step height generally depends on both the superconducting
energy gap and junction parameters. The effect of normal reflections at the
superconductor-semiconductor interface is also examined.
19. A.
Furusaki and M. Ueda
"Semiclassical
Theory Of Small Josephson-Junctions - Solution Of The Master Equation"
Phys.
Rev. B 45 (18), 10576-10596 (1992).
ABSTRACT:
Within a semiclassical approximation and at the weak-coupling limit, where the
charging energy dominates the Josephson coupling energy, the dynamics of
small-capacitance superconducting tunnel junctions can be described by a
stochastic master equation for the probability distribution of junction
charges. We develop a method of solving this equation and obtain an analytic
solution when Cooper-pair, quasiparticle, and Zener tunneling are all present
under an arbitrary Ohmic conductance at zero temperature. We use this solution
to systematically investigate the static and dynamic properties of small
Josephson junctions. The charge distributions, current-voltage characteristics,
and voltage spectra are analytically calculated and numerically evaluated for
wide ranges of parameters. The separate contributions from quasiparticle and
Cooper-pair tunneling to voltage spectra are evaluated and compared based on
their respective sum rules. The linewidths of the resonance peaks for
single-electron tunneling and Bloch oscillations are also discussed.
20. A.
Furusaki and M. Ueda
"Exact
Solution Of The Master Equation For Ultrasmall Normal Tunnel-Junctions"
Phys.
Rev. B 45 (7), 3435-3448 (1992).
ABSTRACT: An
exact solution for the stochastic master equation describing the semiclassical
Coulomb-blockade theory is obtained for an arbitrary shunt resistance at zero
temeprature. This solution is used to systematically evaluate various
quantities characterizing the dynamics of single-electron-tunneling
oscillations. Our solution provides analytic expressions of the voltage spectra
and sum rules.
21. Y. Hida,
S. Imamura, and T. Izawa
"Ring
Resonator Composed Of Low-Loss Polymer Wave-Guides At 1.3-Mu-M"
Electron.
Lett. 28 (14), 1314-1316 (1992).
ABSTRACT: A
channel waveguide ring resonator was successfully fabricated using polymers
synthesised from deuterated methacrylate and deuterated fluoromethacrylate.
Resonance curves with a finesse of 14.8 and an extinction ratio of 0.83 were
obtained at a wavelength of 1.3 mum. The corresponding waveguide loss was
estimated to be 0.10 dB/cm. In addition, the temperature and polarisation
characteristics of the resonance were investigated.
22. Y.
Hirayama
"N-Type
And P-Type Inplane Gated Field-Effect Transistors Directly Written On A
Semiinsulating Gaas Substrate"
Appl.
Phys. Lett. 61 (14), 1667-1669 (1992).
ABSTRACT: A
new type in-plane gated field effect transistor where the semi-insulating
substrate itself is used as a gate insulator region is proposed. n- and p-type
in-plane gated field effect transistors are fabricated on a semi-insulating
GaAs substrate by focused ion beam scanning of Si++ and Be++, respectively.
These in-plane gated field effect transistors are found to operate well at room
temperature.
23. Y.
Hirota, Y. Homma, and K. Sugii
"Clean
And Damage-Free Gaas-Surfaces Prepared By Ultrasonic Running Deionized
Water-Treatment"
Appl.
Surf. Sci. 60-1, 619-624 (1992).
ABSTRACT:
GaAs(001) surfaces treated with ultrasonic running deionized water (URDIW),
after being etched by H2SO4 or NH4OH were examined by using X-ray photoelectron
spectroscopy (XPS) and reflection high-energy electron diffraction (RHEED). XPS
analysis revealed that the arsenic and gallium oxides on chemically etched
surfaces were completely removed by the URDIW treatment. RHEED observation
indicated that the H2SO4-etched GaAs surface shows a streaky (2 X 1) surface
reconstruction pattern at 360-degrees-C and that the NH4OH-etched surfaces show
a (2 x 4) surface reconstruction pattern at 310-degrees-C. These experimental
results indicate that chemically clean GaAs surfaces with little damage can be
produced by URDIW treatment and that the stoichiometry of a URDIW treated surface
can be controlled by varying the etching solutions.
24. T.
Homma, H. Asai, T. Osaka, K. Takei, and Y. Maeda
"Nmr-Study
On Compositional Inhomogeneity In Electroless Deposited Conip Films For
Perpendicular Magnetic Recording"
Chem.
Lett. (9), 1783-1786 (1992).
ABSTRACT:
Compositional inhomogeneity in electroless-deposited CoNiP films with
perpendicular magnetic anisotropy was examined using the spin echo Co-59-NMR
technique for the first time. The existence of a Co-rich component was observed
which was thought to cause the formation of an hcp structure and produce high
perpendicular coercivity, Hc(perpendicular-to). An increment in the Co-rich
component by heat-treatment was also observed which might be an origin of the
increase in Hc(perpendicular-to).
25. Y.
Homma, M. Suzuki, and H. Hibino
"Step
Band Structures On Vicinal Si(111) Surfaces Created By Dc Resistive
Heating"
Appl.
Surf. Sci. 60-1, 479-484 (1992).
ABSTRACT:
DC-heating-induced step bunching is studied using vicinal Si(111) surfaces with
different misorientation angles ranging from 1 to 10-degrees toward [112BAR] in
an ultrahigh vacuum scanning electron microscope. Although the growth rate
depends on the misorientation angle, the bunching structure basically grows in
the same manner on the substrates misoriented from 1 to 8-degrees; faceting of
the surface into (111) terrace regions and step band regions, and then
expansion of terrace regions. The size of the initial facet structure
correlates with the misorientation angle; the period of the structure is
proportional to the misorientation angle. During heating, step band regions
link up with each other forming very straight structures. Thus the surface with
parallel step bands is the final form of the DC-heating-induced step bunching.
The growth rate of the bunching on 1 and 2-degrees surfaces is much higher than
on higher-misorientation-angle surfaces. On a 10-degrees misoriented surface no
DC-heating-induced bunching was observed.
26. K. Hono,
Y. Maeda, J. L. Li, and T. Sakurai
"Direct
Evidence For Compositional Fluctuation In Sputtered Co-Cr Thin-Films"
J.
Magn. Magn. Mater. 110 (3), L254-L258 (1992).
ABSTRACT:
Nano-scale concentration fluctuations in sputtered Co-23 at% Cr magnetic thin
films were analyzed by atom probe field ion microscopy (APFIM). The atom probe
concentration depth profile obtained from the film which was deposited on the W
tip at 200-degrees-C clearly showed that the composition fluctuated
significantly. The concentration of the Cr enriched region was in the range of
30-40 at% Cr, while that of the Cr depleted region was in the range of 5-10 at%
Cr. This result proves that compositional fluctuations are present inside the
grains of the Co-Cr sputtered film as suggested by the TEM observation of the
chrysanthemum-like pattern (CP) structure.
27. A.
Honold, T. Saku, Y. Horikoshi, and K. Kohler
"Optical
Dephasing Of Light-Hole Excitons In Gaas Single Quantum-Wells"
Phys.
Rev. B 45 (11), 6010-6014 (1992).
ABSTRACT:
Picosecond photon-echo experiments were performed on light-hole excitons as
well as heavy-hole excitons in GaAs single quantum wells at low temperatures
and low excitation intensities. The absolute values of the exciton dephasing
times depend on the sample quality but the ratio of the dephasing times of both
exciton types reveals a strong increase in the dephasing rate of light-hole
excitons when the thickness of the quantum well is reduced below 130 angstrom.
This enhanced dephasing of light-hole excitons is due to a Fano-type resonance
when the lowest light-hole exciton state is energetically overlapping with
electron-heavy-hole continuum states. The experimental results are in
reasonable agreement with those of theoretical calculations.
28. T.
Horiuchi, O. Niwa, M. Morita, and H. Tabei
"Stripping
Voltammetry Of Reversible Redox Species By Self-Induced Redox Cycling"
Anal.
Chem. 64 (24), 3206-3208 (1992).
ABSTRACT:
29. R. J.
Horowicz, H. Heitmann, Y. Kadota, and Y. Yamamoto
"Gaas
Microcavity Quantum-Well Laser With Enhanced Coupling Of Spontaneous Emission
To The Lasing Mode"
Appl.
Phys. Lett. 61 (4), 393-395 (1992).
ABSTRACT: We
have observed low-threshold lasing in a GaAs single quantum-well vertical
microcavity. At 4 K the quantum-well emission linewidth is reduced, and the
coupling efficiency-beta of the spontaneous emission to the lasing mode is
improved. The laser threshold pump power obtained for a 200 angstrom GaAs
quantum well pumped by a continuous wave Ti:sapphire laser was 5 mW,
corresponding to 85-mu-W absorbed power. We have compared the experimental
results with the theoretical prediction, and estimated the value of beta to be
10(-2).
30. N.
Hussain, N. Imoto, and R. Loudon
"Quantum-Theory
Of Dynamic Interference Experiments"
Phys.
Rev. A 45 (3), 1987-1996 (1992).
ABSTRACT: We
calculate the first-order interference-fringe visibilities for Mach-Zehnder
interferometers in which the input beam splitter has time-varying reflection
and transmission coefficients. Particular attention is given to single-photon
input states, and it is shown that fringes persist in appropriate conditions
even for a beam splitter that alternates between complete transmission and
complete reflection. The similar behavior found for input coherent and chaotic
light comfirms the single-photon nature of first-order interference. The states
of excitation of the internal arms of the interferometer are derived and
discussed in the context of delayed-choice experiments.
31. A.
Imamoglu and Y. Yamamoto
"Nonclassical
Light Generation By Coulomb Blockade Of Resonant Tunneling"
Phys.
Rev. B 46 (24), 15982-15991 (1992).
ABSTRACT: We
show that the Coulomb blockade of resonant tunneling in semiconductor heterojunctions
creates correlations between single-charge tunneling and single-photon emission
events. When driven by a constant-current source, a mesoscopic p-i-i-i-n
junction generates a regulated single-photon stream by
single-electron-to-single-photon conversion. Under constant-voltage operation,
the photon stream generated by the junction is antibunched and sub-Poissonian.
The single-electron charging energy of the heterostructure has to exceed the
width of the resonant subband and the characteristic energy of the thermal
fluctuations for these correlations to be observable.
32. A.
Imamoglu, Y. Yamamoto, and P. Solomon
"Single-Electron
Thermionic-Emission Oscillations In P-N Microjunctions"
Phys.
Rev. B 46 (15), 9555-9563 (1992).
ABSTRACT: We
show that Coulomb-blockade-type voltage oscillations exist in constant-current
driven p-n microjunctions operated at temperatures below 3 K. These
oscillations occur because of the regulation of the single-electron
thermionic-emission events from the n layer into the p layer. We give an
expression for the average I-V characteristics of the junction in the
Coulomb-blockade regime, which agrees well with the results of the computer
simulations. We also predict the generation of a regulated single-photon stream
from such a p-n junction.
33. S.
Inoue, H. Ohzu, S. Machida, and Y. Yamamoto
"Quantum
Correlation Between Longitudinal-Mode Intensities In A Multimode Squeezed
Semiconductor-Laser"
Phys.
Rev. A 46 (5), 2757-2765 (1992).
ABSTRACT: The
intensity-noise properties of a constant-current-driven multimode semiconductor
laser were studied theoretically and experimentally. It was shown that the
total intensity noise of a pump-noise-suppressed multimode semiconductor laser
was reduced to below the standard quantum limit even though the intensity noise
of each individual mode had large excess intensity noise. This discovery stems
from negative quantum correlations between longitudinal-mode intensities.
34. M. Itoh,
T. Saku, and S. Tarucha
"High-Mobility
Quantum Wires Fabricated By Ga Focused Ion-Beam Shallow Implantation"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 31
(12B), 4487-4491 (1992).
ABSTRACT:
High-mobility quantum wires are fabricated using shallow implantation of a low
energy focused Ga ion beam into a modulation doped AlxGa1-xAs/GaAs
heterostructure. Lowering the implant energy keeps the implanted ions away from
the two-dimensional electron gas and reduces crystallographic damage. The
electron mobility is 5.0 x 10(5) CM2/ V. S for the wires 10 mum long with an
effective width of 0. 152 mum, which is much higher than that for previous
wires. The effective wire width is independently derived from two measurements:
(1) four-terminal conductance at zero-magnetic field and (2) the magnetic
depopulation effect in the Shubnikov-de Haas oscillation. As the implantation
dose decreases, the electron mobility increases with an effective width of more
than 2. 1 -mum, while it is nearly constant for narrower wires. This suggests
the existence of unintentionally implanted neutral Ga atoms and/or stray Ga
ions.
35. F.
Izumi, K. Kinoshita, Y. Matsui, K. Yanagisawa, T. Ishigaki, T. Kamiyama, T.
Yamada, and H. Asano
"The
Crystal-Structure Of The Superconducting Copper-Oxide Carbonate
(Ba1-Xsrx)2cu1+Yo2+2y+Z(Co3)1-Y - Defects In Charge Reservoirs And
Superconductivity"
Physica
C 196 (3-4), 227-235 (1992).
ABSTRACT: The
crystal structure of a new superconductor in the Ba-Sr-Cu-C-O system has been
determined by neutron powder diffraction with the auxiliary use of electron
diffraction and high-resolution transmission electron microscopy. This compound
is a member of a solid solution with the general formula
(Ba1-xSrx)2Cu1+yO2+2y+z(CO3)1-y, where x = 4/9, y = 1/9, and z = 0.10. It is
tetragonal with a space group P42(1)2 or P42(1)mBAR and lattice parameters of a
= 5.56405(18) angstrom and c = 7.8570(4) angstrom. It is closely related in
structure to Sr2CuO2CO3, which is an end member of the solid solution: x = 1, y
= 0, and z = 0. Two-dimensional CuO2 sheets and carbonate slabs,
(Ba1-xSrx)2CuyO2y+z(CO3)1-y, alternate with each other along the [001]
direction. As the formula of the slab shows, about 11% of C atoms are
substituted by excess Cu atoms coordinated to O atoms which amount to 2y + z in
the formula unit. These substitutional and interstitial defects enable hole
carriers to move from the carbonate slab to the CuO2 conduction sheet.
36. Y. Jimbo
and A. Kawana
"Electrical-Stimulation
And Recording From Cultured Neurons Using A Planar Electrode Array"
Bioelectrochem.
Bioenerg. 29 (2), 193-204 (1992).
ABSTRACT:
Planar electrode arrays were fabricated using modern semiconductor technology.
Mouse and chick dorsal root ganglion cells were successfully cultured on the
surface of indium tin oxide electrode patterns. Contact between the neurites
and the substrate electrodes was established by exploiting the surface
properties of the culture substrates to guide neurite outgrowth. The guided
neurites were stimulated electrically using the substrate electrodes and cell
responses were recorded. intracellularly and extracellularly. Depolarization of
the cell membrane as well as generation of action potentials in response to the
stimulation could be observed. The results suggest that this type of planar
electrode array could be a useful tool for non-invasive electrophysiological
measurements.
37. M. Kasu,
H. Ando, H. Saito, and T. Fukui
"Polarized
Photoluminescence Of Fractional Layer Superlattices"
Surf.
Sci. 267 (1-3), 300-303 (1992).
ABSTRACT: The
polarization dependences of photoluminescence of (AlAs)1/2(GaAs)1/2 and
(Al0.5Ga0.5As)1/2(GaAs)1/2 fractional layer superlattices were measured at room
temperature. Anisotropy in light emission was observed for the first time. The
photoluminescence spectra depend on its polarization. This shows that quantum
carrier confinement occurs in the direction parallel to the surface, i.e.,
lateral quantum carrier confinement.
38. M. Kasu
and T. Fukui
"Multiatomic
Steps On Metalorganic Chemical Vapor Deposition-Grown Gaas Vicinal Surfaces
Studied By Atomic Force Microscopy"
Jpn.
J. Appl. Phys. Part 2 - Lett. 31 (7A), L864-L866 (1992).
ABSTRACT: We
studied MOCVD-grown GaAs (001) vicinal surfaces by atomic force microscopy
(AFM) and observed multi-atomic steps (multisteps) of several-monolayers
height. The multisteps become straight as the AsH3 partial pressure increases
and when the misorientation direction is [110BAR]. As growth proceeds, first,
multisteps, i.e., step bunches, form and then the average distance between
multisteps saturates. The multistep straightening and the multistep formation
mechanisms are discussed
39. G. Kido,
S. Yamada, and T. Makimoto
"Subband
Structure Of 2-Dimensional Electrons At Double Silicon-Doped Atomic Layers In
Gaas"
Physica
B 177 (1-4), 433-436 (1992).
ABSTRACT:
Longitudinal and transverse magnetoresistance experiments were carried out on
GaAs with two impurity-doped planes in steady high magnetic fields up to 30 T.
A large oscillation was observed in the field range higher than 10 T. The
double Si-doped planes behave as a single well even for 15 nm separation of the
atomic planes.
40. K.
Kinoshita, F. Izumi, T. Yamada, and H. Asano
"Structure
Refinements Of Superconducting And Nonsuperconducting La1.82ca1.18cu2o+/-Delta
From Neutron-Diffraction Data"
Phys.
Rev. B 45 (10), 5558-5562 (1992).
ABSTRACT: The
crystal structures of superconducting and nonsuperconducting La1.82Ca1.18Cu2O6
+/- delta synthesized under O2 pressures of 400 and 2 atm were refined by
Rietveld analysis of neutron-powder-diffraction data. These samples contained
no impurities and their observed and calculated diffraction patterns were in
excellent agreement. In both samples, Ca and La preferentially occupied,
respectively, a 2a site in eightfold coordination and a 4e site in ninefold
coordination; a slightly higher ordering was observed in the superconducting
compound. An apical oxygen site was almost fully occupied. A trace of excess
oxygen between two CuO2 planes was detected in the superconducting compound.
Cu-O(1) and Cu-O(2) bond lengths differed a little between the two samples.
Increases in cation ordering and in interstitial oxygen might be important
factors determining superconductivity in this system.
41. K.
Kinoshita, H. Shibata, and T. Yamada
"Crystal-Structure
And Superconductivity In La1.85sr0.16ca0.99cu2o5.93+Delta"
Phase
Transit. 37 (2-3), 121-130 (1992).
ABSTRACT:
42. K.
Kinoshita and T. Yamada
"Superconductivity
And Antiferromagnetism In La2-Xca1+Xcu2o6+/-Delta And
La2-Xsrxcacu2o6+/-Delta"
Phys.
Rev. B 46 (14), 9116-9122 (1992).
ABSTRACT:
La2CaCu2O6 can be made superconducting by doping Ca or Sr in the form of
La2-x(Sr,Ca)xCaCu2O6+delta and by synthesis under high O2 pressures of more
than 4 atm. Superconducting properties of La2-xCa1+xCu2O6+/-delta (0.08
less-than-or-equal-to x less-than-or-equal-to 0.25) and La2-xSrxCaCu2O6+/-delta
(0.07 less-than-or-equal-to x less-than-or-equal-to 0.23) as functions of
composition (x) and oxygen partial pressure during synthesis (P(O2) up to 400
atm) were investigated by measuring their electrical resistivity and magnetic
susceptibility. In both compounds, the superconducting transition temperature
(T(c)) increased with increasing x and P(O2), and showed almost the same
maximum T(c) (zero) of about 51 K at the solubility limit of Ca or Sr in La (x
almost-equal-to 0. 25) with P(O2) at 400 atm, although at a lower P(O2), T(c)
(zero) was higher in a Sr-doped compound than that of a Ca-doped compound.
Nonsuperconducting or weakly superconducting La2-xCa1+xCu2O6+/-delta and
La2-xSrxCaCu2O6+/-delta synthesized under oxygen partial pressures between 0.2
and 10 atm showed cusps in their magnetic susceptibility at around 25 K, which
may result from three-dimensional (3D) antiferromagnetic ordering. The
superconductivity of these compounds may appear as a result of the frustration
of such 3D antiferromagnetic correlation as with other copper oxide
superconductors.
43. K.
Kinoshita and T. Yamada
"High-Pressure
Synthesis Of Superconducting
(Ba1-Xsrx)2cu1+Yo2+2y+Delta(Co3)1-Y(0.35-Less-Than-Or-Equal-To-X-Less-Th An-Or-Equal-To-0.6,Y-Approximate-To-0.1)"
Jpn.
J. Appl. Phys. Part 2 - Lett. 31 (7A), L832-L834 (1992).
ABSTRACT: A
new copper-oxide superconductor containing carbon
(Ba1-xSrx)2Cu1+xO2+2y+delta(CO3)1-y (0.35 less-than-or-equal-to x
less-than-or-equal-to 0.6, y almost-equal-to 0.1), which is structurally
related to Sr2CuO2CO3, was synthesized under high oxygen pressures of more than
5 atm. The onset temperature for superconduction T(c)(onset) increased with
oxygen partial pressure (P(O2)) during synthesis. Optimum P(O2) was about 50
atm and (Ba0.55Sr0.45)2Cu1.1O2.2+delta(CO3)0.9 synthesized under 50 atm O2,
showed a T(c)(onset) of about 40 K and a T(c)(zero) of about 26 K.
44. K.
Kinoshita and T. Yamada
"A
New Copper-Oxide Superconductor Containing Carbon"
Nature 357
(6376), 313-315 (1992).
ABSTRACT:
SUPERCONDUCTIVITY in the high-transition-temperature (high-T(c)) copper oxide
superconductors seems to arise from layers of copper-oxygen squares, pyramids
or octahedra. Recently the compound Sr2CuO2CO3 was found to contain layers of
CuO6 octahedra 1 (Fig. 1), suggesting that it might be made superconducting by
appropriate doping. But the presence of carbonate as an impurity is known to
degrade the superconducting properties of materials such as YBa2Cu3O7-delta'
and YBa2Cu4O8 (refs 2,3), much effort having been made to minimize residual
carbon in these compounds by optimizing processing methods 4. It is thus of
some interest to see whether Sr2CuO2CO3 can be made superconducting despite the
carbonate ions incorporated in the structure. Here we report the synthesis, at
50 atm oxygen partial pressure, of superconducting
(BaxSr1-x)2Cu1+yO2+2y+delta(CO3)1-y (0.4 less-than-or-equal-to x
less-than-or-equal-to 0.65, y almost-equal-to 0.1), with T(c) (onset) up to
approximately 40 K and zero resistance at up to approximately 26K. The crystal
structure contains CuO2 sheets alternating with (BaxSr1-x)2CuyO2y+delta(CO3)1-y
slabs, which serve as charge reservoir layers: substitution of approximately
10% copper for carbon in the slabs introduces holes into the CuO2 sheets,
making the compound superconducting.
45. N.
Kobayashi and Y. Kobayashi
"Insitu
Control Of Heterointerface Quality In Movpe By Surface Photoabsorption"
J.
Cryst. Growth 124 (1-4), 525-530 (1992).
ABSTRACT: Exchange
reaction of Group V atoms is in situ monitored on a submonolayer scale during
the MOVPE growth of pseudomorphic InAs/InP heterostructures on (001) InP
substrate by the surface photo-absorption (SPA) method. When arsine was
supplied onto the In surface of InP above 360-degrees-C, the substitution
between As atoms of impinging AsH3 molecules and P atoms of InP surface was
detected as a change in surface reflectivity. The reaction proceeded to about
0.4 monolayer exchange at 400-degrees-C, and was suppressed to less than 0.1
monolayer at 350-degrees-C. In contrast, the exchange between P atoms of
impinging PH3 and As atoms of InAs surface was less than 0.1 monolayer below
400-degrees-C. To verify the formation of a metallurgically abrupt heterointerface,
InAs/InP single quantum wells with 1-5 monolayers were grown at 350-degrees-C,
and were characterized by transmission electron microscopy and
photoluminescence. Atomic layer epitaxy was used to control precisely the InAs
well thickness with an accuracy of one monolayer. A sharp and an intense
quantum well photoluminescence was observed with a reasonable shift of emission
energy due to the quantum size effect up to five InAs monolayers, indicating
that metallurgically abrupt and atomically flat heterointerfaces were
fabricated as designed.
46. N.
Kobayashi, Y. Kobayashi, Y. Yamauchi, and Y. Horikoshi
"Insitu
Optical Monitoring Of The Decomposition Process Of Gaseous Sources In
Metal-Organic Chemical Vapor-Deposition And Atomic Layer Epitaxy"
Appl.
Surf. Sci. 60-1, 544-552 (1992).
ABSTRACT: We
apply surface photo-absorption (SPA) to study the heterogeneous decomposition
of Group-III sources on a substrate surface during metal-organic chemical vapor
deposition (MOCVD). We first show the substrate temperature (T(s)) dependence
of the SPA signal at the supply of a Group-III source to a Group-V stabilized
surface. The decomposition onset temperature obtained from the rising of the
SPA signal, agrees well with the starting temperature of growth. Triethyl Al,
Ga and In sources have lower onset temperatures than the corresponding
trimethyl sources. A new Al source, trimethylamine alane, decomposes below
200-degrees-C. The region of atomic layer epitaxy (ALE) appears as a shoulder
or a plateau in the neighborhood of decomposition onset. In this region, the
surface is saturated by adsorption of the trimethyl source, and it is concluded
that the self-limiting growth rate is caused by the intermolecular repulsion
between impinging metal-organic molecules and CH3 groups metastably terminating
the growth surface. SPA allows real-time control of the ALE process, because it
distinguishes a metastable CH3-terminated surface from a metal one, and the
growth parameters for obtaining CH3 termination are readily determined.
47. N.
Kobayashi and Y. Yamauchi
"Enhancement
Of Ash3 Decomposition On Highly Doped P-Gaas Surfaces"
J.
Cryst. Growth 124 (1-4), 44-48 (1992).
ABSTRACT:
Surface photo-absorption (SPA) was used to study the effect of semiconductor
surface potential on the heterogeneous decomposition of source molecules in
MOVPE. The decomposition rate of AsH3 was enhanced on the Ga surface of p-GaAs
in proportion to a square root of the carrier concentration. In contrast, an
enhancement on Si doped n-GaAs was negligible up to 2 X 10(18) cm-3. The
decomposition activation energy was almost independent of the conduction type
and of the carrier concentration. From these results, the enhancement of AsH3
decomposition on p-GaAs might be caused by an increase in the mean lifetime of
AsH3 adsorption on the Ga surface of p-GaAs due to an attractive force between
the dipole of the AsH3 molecule and the surface electric field. For the Group
III source, a preliminary study by the scattered light method which detects the
Ga droplet formation showed that the decomposition of triethylgallium was
enhanced on the As surface of n+-GaAs in the kinetically controlled temperature
region.
48. Y.
Kobayashi and N. Kobayashi
"Insitu
Interface Control Of Pseudomorphic Inas/Inp Quantum-Well Structure Growth By
Surface Photoabsorption"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 31
(12A), 3988-3994 (1992).
ABSTRACT: The
exchange reaction of group V atoms was monitored in situ by surface
photo-absorption on a submonolayer scale during metalorganic vapor phase
epitaxial growth of pseudomorphic InAs/InP heterostructure on (001) InP
substrates. About a 0.4-monolayer As/P exchange reaction was observed after
arsine was supplied at 0.2 mumol/s onto the In surface of InP at a substrate
temperature (T(s)) of 400-degrees-C. At a T(s) of 350-degrees-C, this As/P
exchange reaction was suppressed to less than 0.1 monolayer. In contrast, the
P/As exchange reaction was less than 0.1 monolayer below 400-degrees-C. The
benefits of in situ control were shown by growing pseudomorphic InAs/InP single
and multiple quantum wells with 1-12 InAs well layers at T(s)=350-degrees-C and
characterizing them by cross sectional transmission electron microscopy,
photoluminescence, and double crystal X-ray diffraction. Metallurgically abrupt
and atomically flat heterostructures without dislocations were grown to 10
monolayer (ML) of InAs well, which corresponds to the critical layer thickness.
49. Y.
Kobayashi and N. Kobayashi
"Growth-Rate
Self-Limitation Mechanism In Inp Atomic Layer Epitaxy Studied By Surface
Photoabsorption"
Jpn.
J. Appl. Phys. Part 2 - Lett. 31 (2A), L71-L73 (1992).
ABSTRACT: The
pyrolysis of trimethylindium (TMI) and phosphine (PH3) on an (001) InP surface
is studied by surface photo-absorption. In the same manner as the pyrolysis of
trimethylgallium on GaAs, self-limitation is observed in the change in
reflectivity when TMI is supplied to a P-stabilized surface at 350-degrees-C.
This result indicates that the surface is saturated by TMI adsorption to form a
CH3-terminated In surface. H-2 purging after TMI adsorption increases the
reflectivity further to the level of a metal surface with an In monolayer,
indicating that CH3 groups desorb during purging. This paper also finds the
pyrolysis of PH3 on a CH3-terminated In surface is much slower than on In metal
surface. The growth rate is self-limited to less than one monolayer per cycle
in InP atomic layer epitaxy because the surface is not completely transformed
to a P surface during PH3 supply, as PH3 pyrolysis is slow on a CH3-terminated
In surface. The growth rate approaches one monolayer per cycle when PH3 is
supplied to an In metal surface produced by CH3 desorption.
50. Y.
Kobayashi and K. Sugii
"Thermal-Decomposition
Of Very Thin Oxide Layers On Si(111)"
J.
Vac. Sci. Technol. A-Vac. Surf. Films 10 (4),
2308-2313 (1992).
ABSTRACT: We
investigate the thermal decomposition and desorption of very thin oxide layers
prepared on Si (111) by oxygen adsorption as well as by chemical treatments.
The oxides are examined by Auger electron spectroscopy, thermal desorption
spectroscopy, and atomic force microscopy. The decomposition mechanism changes
drastically at an oxide thickness of approximately 6 angstrom; the
decomposition temperature depends on the formation method for oxides thicker
than 6 angstrom, but the dependence disappears for oxides thinner than 6
angstrom. The former result can be qualitatively interpreted by the difference
in SiO diffusivity between the oxides. The latter suggests that the
decomposition rate is governed by reactions at the oxide/Si interface because
the oxide layer is so thin that diffusion is not the dominant factor. The
possibility of thermally removing the thin oxide layer in a dry oxygen/Si
system for layer-by-layer etching or "monolayer peeling" is also
discussed.
51. J. T.
Kucera, L. M. Rubin, K. Uwai, J. D. Perkins, J. M. Graybeal, T. P. Orlando, J.
B. Vandersande, A. Roshko, and J. Moreland
"Fabrication
Of Nanometer Smooth Bi2sr2cacu2o8+ Delta Films By Reactive Cosputtering From
Elemental Targets With Pure Ozone"
Physica
C 192 (1-2), 23-30 (1992).
ABSTRACT: We
describe the fabrication of superconducting Bi2Sr2CaCu2O8+delta thin films
having root-mean-square surface roughnesses of less than 5 nm as determined by
scanning tunneling microscopy. Films are deposited in-situ by RF and DC triode
magnetron sputtering from elemental metallic targets in the presence of pure
ozone. As deposited, these films have transition temperatures as high as 68 K
and zero-field critical current densities exceeding 10(6) A/cm2 at 4.2 K. The
transition temperatures can be increased to 80 K by post-deposition annealing
with only a slight increase in surface roughness.
52. K. Maezawa,
T. Mizutani, and S. Yamada
"Effective
Mass And Ground-State Of Alas Quantum-Wells Studied By Magnetoresistance
Measurements"
J.
Appl. Phys. 71 (1), 296-299 (1992).
ABSTRACT:
Transport properties of electrons confined in AlAs quantum wells were studied
using low temperature magnetoresistance measurement. The structure used is
quantum wells consisting of AlAs channel layers sandwiched by Si-doped
Al0.45Ga0.55As barrier layers. This structure enables us to confine electrons
in the X valleys of AlAs. The electron confinement in the AlAs quantum wells
were confirmed by a mobility enhancement at low temperatures. Magnetoresistance
measurements showed clear Shubnikov-de Haas oscillations for the magnetic field
parallel to the growth direction. A large effective mass of (0.55 +/- 0.05) m0,
which is close to square-root m(t)m(l) (m(t):transverse effective mass,
m(l):longitudinal effective mass), was obtained from the temperature dependence
of the oscillations. This indicates that the ground state is X(x), X(y), even
though X(z) was expected to be the ground state due to its large effective mass
parallel to the growth direction. This changeover of AlAs X valley states can
most likely be attributed to a strain-induced energy shift caused by the small
lattice mismatch between GaAs and AlAs.
53. T.
Makimoto and S. S. Chang
"Carbon
Modulation-Doped P-Algaas/Gaas Heterostructures Grown By Metalorganic Chemical
Vapor-Deposition"
Jpn.
J. Appl. Phys. Part 2 - Lett. 31 (6B), L797-L798 (1992).
ABSTRACT:
Carbon atoms are used as a p-type dopant for modulation-doped p-AlGaAs/GaAs
heterostructures grown by metalorganic chemical vapor deposition. Carbon
impurities are effectively doped into AlGaAs layers by flow-rate modulation
epitaxy, which is a modified method of metalorganic chemical vapor deposition.
A mobility of 6.0 x 10(4) cm2/V.s is obtained at 13 K for a sheet carrier
concentration of 4.1 x 10(11) cm-2, indicating that a high quality
two-dimensional hole gas is realized by abrupt heterointerfaces and sharp carbon
doping profiles.
54. S.
Masuyama and S. Naito
"Deciding
Whether Graph-G Has Page Number One Is In Nc"
Inf.
Process. Lett. 44 (1), 7-10 (1992).
ABSTRACT:
Based on a forbidden subgraph characterization of a graph to have one page, we
develop a polylog time algorithm to tell if a given graph G has page number
one, with polynomial number of processors, clarifying this problem to be in NC.
55. N.
Mitani and S. Kurihara
"Marginal
Fermi-Liquid Theory And Renormalization Effects"
Physica
C 192 (1-2), 230-236 (1992).
ABSTRACT:
Marginal Fermi-liquid theory proposed by Varma et al. is based on an assumption
concerning the imaginary part of the polarization propagator. We investigate
the consequence of this assumption paying full respect to the Ward-Takahashi
identity, and find that the vertex corrections are of vital importance. We
confirm the validity of the marginal Fermi-liquid picture at high energy scale,
where only the lowest order logarithmic correction is important. However, our
result at the low-energy region is radically different from the marginal Fermi
liquid theory, in the sense that the quasi-particle mass, strength of its pole,
and the jump in the momentum distribution all remain finite at the Fermi level.
This means that the Varma et al. assumption does not break the Fermi-liquid
picture, as far as the low-energy excitations are concerned.
56. M.
Mitsunaga
"Time-Domain
Optical-Data Storage By Photon-Echo"
Opt.
Quantum Electron. 24 (10), 1137-1150 (1992).
ABSTRACT:
Principles and applications of time-domain optical data storage using
stimulated photon echo are briefly reviewed. Special emphasis is laid upon the
comparison of this memory with holography; both memories use the interference
between two optical waves. Some new experimental developments are introduced
using samples of europium-ion-doped crystals, one of the most promising candidates
in time-domain data storage. Some other topics, such as ultrafast data storage,
time-domain data processing, and time- and spatial-image storage using photon
echo, are also discussed.
57. M.
Mitsunaga, T. Takagahara, R. Yano, and N. Uesugi
"Excitation-Induced
Frequency-Shift Probed By Stimulated Photon-Echoes"
Phys.
Rev. Lett. 68 (21), 3216-3219 (1992).
ABSTRACT: A
stimulated photon-echo study has verified the instantaneous shift
(less-than-or-equal-to 1 MHz) and subsequent restoration (approximately 2 ms)
of the transition frequency of an impurity ion in a solid when its neighboring
ions are exposed to pulsed optical excitation. Experiments were conducted by
monitoring the echo intensity for the F-7(0)-5D0 transition of Eu ions in one
site of Y2SiO5, while exciting the other site. A photon-echo theory taking
account of the stochastic frequency recovery is developed to explain the
observations.
58. M.
Mitsunaga, R. Yano, and N. Uesugi
"Stimulated-Photon-Echo
Spectroscopy.2. Echo Modulation In Pr3+ Yalo3"
Phys.
Rev. B 45 (22), 12760-12768 (1992).
ABSTRACT:
Stimulated-photon-echo measurements as a function of both the first-to-second
(tau) and the second-to-third (T) pulse separations were conducted to study the
echo-modulation behavior for the H-3(4)-D-1(2) transition of a cryogenic
Pr3+:YAlO3 sample. When T is shorter than the excited-state lifetime T1, deep
echo modulations along both the tau and T axes are observed, the frequencies of
which correspond to the excited-state sublevel splittings. When T exceeds T1,
the modulation is still observed, although only along the tau-axis. A
density-matrix theory is developed in a perturbative manner to explain these
coherent dynamical properties. The numerically simulated three-dimensional
plots of the echo intensity versus tau and T are presented, predicting quite
satisfactorily the seemingly complicated experimental modulation patterns.
59. F.
Mokhtarian and A. K. Mackworth
"A
Theory Of Multiscale, Curvature-Based Shape Representation For Planar
Curves"
IEEE
Trans. Pattern Anal. Mach. Intell. 14 (8), 789-805 (1992).
ABSTRACT:
This paper presents a multiscale, curvature-based shape representation
technique for planar curves that satisfies several criteria that are considered
necessary for general-purpose shape representation methods. As a result, the
representation is suitable for tasks that call for recognition of a noisy curve
of arbitrary shape at an arbitrary scale or orientation. The method rests on
the concept of describing a curve at varying levels of detail using features
that are invariant with respect to transformations that do not change the shape
of the curve. Three different ways of computing the representation are
described in this paper. These three methods result in three different representations:
the curvature scale space image, the renormalized curvature scale space image,
and the resampled curvature scale space image. The process of describing a
curve at increasing levels of abstraction is referred to as the evolution or
arc length evolution of that curve. Several evolution and arc length evolution
properties of planar curves are described in this paper. Some of these results
show that evolution and arc length evolution do not change the physical
interpretation of planar curves as object boundaries, and some characterize
possible behaviors of planar curves during evolution and arc length evolution.
Others impose constraints on the location of a planar curve as it evolves.
Together, these results provide a sound theoretical foundation for the
representation methods introduced in this paper.
60. M.
Morita, T. Horiuchi, and H. Tabei
"Differential
Pulse Voltammetry Of Reversible Redox Species At Interdigitated Array
Electrodes"
J.
Electroanal. Chem. 322 (1-2), 191-201 (1992).
ABSTRACT: Differential
pulse (DP) voltammetry of reversible redox species has been measured with
interdigitated array (IDA) electrodes in single and dual potentiostated modes.
The concentration profile near the electrode was renewed rapidly because of
non-planar diffusion toward the electrode. Therefore, no depletion effect was
observed in either mode when the waiting time was 0.4 or 5 s. The pulse
electrolysis time and the applied pulse potential dependence of the peak
currents in the single mode follow conventional DP voltammetry with a macro
electrode. However, constant peak currents were observed in the dual mode which
depended on the applied pulse potential and the average diffusion distance
calculated from the IDA electrode configuration. The current in a DP voltammogram
with IDA electrodes in the dual mode can be expressed as (DELTA-i)max =
i(lim)[(1 - sigma)/(1 + sigma)] where i(lim) is the limiting current in the
cyclic voltammogram with the IDA in the dual mode. The sensitivity for
ferrocene derivatives was improved up to 2 nmol/dm3 as a result of the high
collection efficiency and redox cycling.
61. H.
Murase
"Surface
Shape Reconstruction Of A Nonrigid Transparent Object Using Refraction And
Motion"
IEEE
Trans. Pattern Anal. Mach. Intell. 14 (10), 1045-1052 (1992).
ABSTRACT: The
appearance of a pattern behind a transparent, moving object is distorted by
refraction at the moving object's surface. This paper describes an algorithm
for reconstructing the surface shape of a nonrigid transparent object, such as
water, from the apparent motion of the observed pattern. This algorithm is
based on the optical and statistical analysis of the distortions. It consists
of the following parts: 1) extraction of optical flow, 2) averaging of each
point trajectory obtained from the optical flow sequence, 3) calculation of the
surface normal using optical characteristics, and 4) reconstruction of the
surface. The algorithm is applied to both synthetic and real images to
demonstrate its performance.
62. K.
Nakamura and H. Nakano
"Faraday-Rotation
In Cd1-Xmnxte/Cd1-Yznyte Superlattice"
J.
Phys. Soc. Jpn. 61 (4), 1390-1398 (1992).
ABSTRACT: The
present paper is concerned with an experimental study of Faraday rotation in a
Cd0.89Mn0.11Te/Cd0.61Zn0.39Te superlattice at 300 K and 4.2 K. As the width of
Cd0.89Mn0.11Te well decreases, a lying-S shaped dispersion of the Faraday
rotation spectrum, which is consistent with a predominant exciton transition of
\ 3/2, +/- 3/2 > to \ 1/2, +/- 1/2 >, shifts toward a higher photon energy,
and the peak value of the dispersion spectrum becomes larger than that for the
Cd0.89Mn0.11Te thin film. In the superlattice systems, we also observed a
Faraday rotation spectrum consistent with the exciton transition of \ 3/2, +/-
1/2 > to \ 1/2, +/- 1/2 > at a higher photon energy. The shift of the
energy-band gap due to the lattice-mismatch is calculated for this system on
the basis of the model of free standing strained superlattice. The positions of
calculated energy in the dispersion spectrum are in good agreement with
experimental results.
63. J.
Nakata, M. Taniguchi, and K. Takahei
"Direct
Evidence Of Er Atoms Occupying An Interstitial Site In Metalorganic Chemical
Vapor Deposition-Grown Gaaser"
Appl.
Phys. Lett. 61 (22), 2665-2667 (1992).
ABSTRACT: Er
doped GaAs grown by metalorganic chemical vapor deposition is studied by the
Rutherford backscattering channeling method. We directly confirmed, for the
first time, that Er ions occupy a somewhat displaced tetrahedral interstitial
site, rather than a substitutional site, in the GaAs host. This is concluded
from the observation of a remarkable peak of the doped Er ions caused by the
flux peaking effect in the [110] channeling direction. Also leading to this
conclusion is the fact that the ratios of the [111] and [100] channeling yields
to the random yields for Er ions were larger than those for the GaAs host.
Moreover, we observe peak shifts towards the higher energy region in the [110]
spectra compared to the random spectra. This is due to the lower stopping power
of He ions in the GaAs host in the channeling direction than in the random
direction. We deduce the strikingly small stopping power ratio of the [110] to
the random incidence is also discussed.
64. S.
Nakata
"Observation
Of Tunneling Phenomena And The Charging Effect Through Small Constricted
Regions In Semiconductors Fabricated With A Focused Ion-Beam At 4.2-K"
Phys.
Rev. B 46 (20), 13326-13330 (1992).
ABSTRACT:
Small tunnel barrier were formed on AlxGa1-xAs/GaAs by focused-ion-beam
implantation. The samples were then measured with dc current at 4.2 K, and the
I-V curves revealed two distinct regions depending on applied bias: a tunneling
region at small bias voltage and a region where thermal current over the
barrier is dominant at large bias voltage. A dip in the dI/dV curve was
observed in the tunneling region in the source-drain voltage (V(SD)) range from
- 5 to 5 mV. In a different sample, periodic and reproducible staircaselike
steps with a periodicity DELTAV(SD) of 35 mV were observed. This phenomenon is
related to he Coulomb staircase, which occurs when the capacitance of a quantum
dot is very small.
65. S.
Nishida and T. Sato
"Positive
Motion After-Effect Induced By Bandpass-Filtered Random-Dot Kinematograms"
Vision
Res. 32 (9), 1635-1646 (1992).
ABSTRACT:
Using spatially filtered random-dot kinematograms (RDK) with a 1 octave
bandwidth, the duration and direction of motion aftereffect (MAE) were measured
while varying step displacement, and the results were compared to those for
motion direction discrimination. We found that MAE and motion discrimination
show quite different dependencies on displacement. At displacements around 0.5
cycles of the lowest frequency, while motion discrimination was still almost
perfect, normal MAE vanished and MAE in the same direction as that of the
adapting stimuli, which we name "positive MAE", was observed. Similar
results were obtained for both 1- and 2-dimensional filtered patterns. A
theoretical examination based on the Fourier components of the stimuli showed
that the displacement dependency of MAE is predictable in terms of adaptation
of first-order detectors, but that of motion discrimination is not. The present
results indicate that direction perception and MAE for bandpass RDKs are
mediated at least partially by separate mechanisms, and that direction
perception at larger displacements is mediated by the second-order mechanism
which detects movement of contrast modulation in the image.
66. J.
Nitta, T. Akazaki, H. Takayanagi, and K. Arai
"Transport-Properties
In An Inas-Inserted-Channel In0.52al0.48as/In0.53ga0.47as Heterostructure
Coupled Superconducting Junction"
Phys.
Rev. B 46 (21), 14286-14289 (1992).
ABSTRACT:
Supercurrent is observed in a superconductor-semiconductor-superconductor
(S-Sm-S) junction using a two-dimensional-electron-gas system in an
InAs-inserted-channel In0.52Al0.48As/In0.53Ga0.47As heterostructure. The
temperature dependence of the supercurrent cannot be explained by a simple
exponential expression, but is here explained in terms of the clean-limit
theory, taking account of the higher-order effect of the coherence length. The
differential resistance of the junction shows clear subharmonic energy-gap
structures due to multiple Andreev reflection since the phase coherence is
maintained during the Andreev-reflection process. The Cooper pair transport
explained by the clean-limit theory is attributed to the fact that the mean
free path is longer than the coherence length and the length between the
superconducting electrodes.
67. K.
Nozawa and Y. Horikoshi
"Low
Threading Dislocation Density Gaas On Si(100) With Ingaas/Gaas Strained-Layer
Superlattice Grown By Migration-Enhanced Epitaxy"
J.
Electron. Mater. 21 (6), 641-645 (1992).
ABSTRACT:
This paper reports a promising approach for reducing the density of threading
dislocations in GaAs on Si. InxGa1-xAs/GaAs strained-layer superlattices (SLSs)
grown by migration-enhanced epitaxy at 300-degrees-C on GaAs/Si acted as
barriers to threading dislocations. Unlike conventional high-temperature-grown
SLSs, the low-temperature-grown SLSs were hardly relaxed by the formation of
misfit dislocations at GaAs/SLS interfaces, and this allowed them to accumulate
considerable strain. New threading dislocation generation due to the misfit
dislocation was also suppressed. These factors caused effective bending of
threading dislocations and significantly reduced the dislocation density. For
the samples that had an SLS with x = 0.3, the average etch-pit density was 7 X
10(4) cm-2, which is comparable to that of GaAs substrates.
68. M. Ogawa
"Chew
Theorem Revisited - Uniquely Normalizing Property Of Nonlinear Term
Rewriting-Systems"
Lect.
Notes Comput. Sci. 650, 309-318 (1992).
ABSTRACT:
This paper gives a purely syntactical proof, based on proof normalization
techniques, of an extension of Chew's theorem. The main theorem is that a
weakly compatible TRS is uniquely normalizing. Roughly speaking, the weakly
compatible condition allows possibly nonlinear TRSs to have nonroot overlapping
rules that return the same results. This result implies the consistency of
CL-pc which is an extension of the combinatory logic CL with parallel-if rules.
69. T.
Ogawa, A. Furusaki, and N. Nagaosa
"Fermi-Edge
Singularity In One-Dimensional Systems"
Phys.
Rev. Lett. 68 (24), 3638-3641 (1992).
ABSTRACT: The
Fermi-edge singularity in optical spectra is studied theoretically using the
Tomonaga-Luttinger model for one-dimensional (1D) systems. Its critical
exponent is obtained analytically for an arbitrary mass of a valence hole
taking into account the electronic correlation. The exponent is found to be
independent of the hole dynamics in 1D, which is in striking contrast to the 2D
and 3D cases. Weak repulsive interaction among the conduction electrons
sharpens the power-law peak in the edge spectrum.
70. T. Ogawa
and T. Takagahara
"Excitonic
Absorption-Spectra And Sommerfeld Factors Of One-Dimensional Systems"
Surf.
Sci. 263 (1-3), 506-511 (1992).
ABSTRACT: We
investigate theoretically optical absorption spectra near a band edge for
one-dimensional (1D) semiconductors with a direct band gap, taking 1D
Wannier-type exciton effects into account. The Sommerfeld factor, which is the
absorption intensity ratio of the continuum exciton to the free electron-hole
pair above the band edge, is found to be smaller than unity for an allowed
transition in striking contrast to the three- and two-dimensional cases. This
peculiar feature is interpreted in terms of the anomalously strong concentration
of the oscillator strength on the lowest discrete exciton state.
71. T. Ohno,
K. Shiraishi, and T. Ogawa
"Intrinsic
Origin Of Visible-Light Emission From Silicon Quantum Wires -
Electronic-Structure And Geometrically Restricted Exciton"
Phys.
Rev. Lett. 69 (16), 2400-2403 (1992).
ABSTRACT: We
theoretically investigate excitonic effects on the optical properties of
silicon quantum wires, based on ab initio electronic structure calculations.
The Si wires have a direct, allowed band gap in the visible energy range and
exhibit a strong optical anisotropy. Taking into account the electron-hole
Coulomb interaction, the geometrical restriction of excitons dramatically
enhances the oscillator strength of the optical transitions. Comparisons with
recent experimental results are also made.
72. M. Okada
"An
Efficient One-Pass Search Algorithm For Parsing Spoken Language"
IEICE
Trans. Fundam. Electron. Commun. Comput. Sci. E75A
(7), 944-953 (1992).
ABSTRACT:
Spoken language systems such as speech-to-speech dialog translation systems
have been gaining more attention in recent years. These systems require full
integration of speech recognition and natural language understanding. This
paper presents an efficient parsing algorithm that integrates the search
problems of speech processing and language processing. The parsing algorithm we
propose here is regarded as an extension of the finite-state-network directed,
one-pass search algorithm to one directed by a context-free grammar with
retention of the time-synchronous procedure. The extended search algorithm is
used to find approximately globally optimal sentence hypotheses; it does not
have overhead which exists in, for example, hierarchical systems based on the
lattice parsing approach. The computational complexity of this search algorithm
is proportional to the length of the input speech. As the search process in the
speech recognition can directly take account of the predictive information in
the sentence parsing, this framework can be extended to spoken language systems
which deal with dynamically varying constraints in dialogue situations.
73. Y. Okada
and M. Hayashi
"Graph
Rewriting-Systems And Their Application To Network Reliability-Analysis"
Lect.
Notes Comput. Sci. 570, 36-47 (1992).
ABSTRACT: We
propose a new kind of Graph Rewriting Systems (GRS) that provide a theoretical
foundation for using the reduction methods to analyze network reliability, and
give the critical pair lemma in this paper.
74. N.
Osaka, K. Kakehi, S. Iai, and N. Kitawaki
"A
Model For Evaluating Talker Echo And Sidetone In A Telephone Transmission
Network"
IEEE
Trans. Commun. 40 (11), 1684-1692 (1992).
ABSTRACT: We
are studying an objective evaluation model called OPINE (overall performance
index model for network evaluation) for telephone transmission quality. The
model estimates an MOS (mean opinion score) by summing psychological values on
independent psychological factors, given the physical values of fundamental
listening factors such as loss and noise. For the model to incorporate new
talking factors such as talker echo and sidestone, evaluation characteristics
are studied when both listening and talking factors are present in a telephone
transmission system. This paper focuses on the interaction of the listening and
talking factors and shows experimentally that these talking factors are
independent of fundamental listening factors. From these results, an extended
OPINE is proposed by establishing new psychological factors: talker echo and
sidestone. The estimated MOS for composite conditions of listening and talking
factors agrees well within the confidence interval of subjective MOS deviation.
In addition, the results of comparison with another model are shown.
75. K.
Otsuka
"Highly
Sensitive Measurement Of Doppler-Shift With A Microchip Solid-State Laser"
Jpn.
J. Appl. Phys. Part 2 - Lett. 31 (11A), L1546-L1548 (1992).
ABSTRACT:
Intensity modulation of a LiNdP4O12 microchip solid-state laser by reflected
scattered light from a moving object is investigated experimentally and
numerically. Ultra-high sensitivity detection of Doppler-shift and application
to a laser velocity meter are demonstrated.
76. K.
Otsuka and J. L. Chern
"Dynamic
Spatial-Pattern Memory In Globally Coupled Lasers"
Phys.
Rev. A 45 (11), 8288-8291 (1992).
ABSTRACT: The
chaotic dynamics found in globally coupled modulated laser systems have been
switched into stable orbits, including antiphase periodic states and clustered
states, by an injection-seeding method. Direct assignment to desired factorial
periodic orbits has been demonstrated. Self-induced switching among
destabilized clustered states (chaotic itinerancy) in the transition process
from clustered states to global chaos has also been found.
77. K.
Otsuka and J. L. Chern
"Synchronization,
Attractor Fission, And Attractor Fusion In A Globally Coupled Laser
System"
Phys.
Rev. A 45 (7), 5052-5055 (1992).
ABSTRACT: A
globally coupled class-B laser array with incoherent feedback is proposed for
exploring the complex dynamics of dynamical systems with the highest
connectivity. This feedback shows a fundamental characteristic, information
lag, and results in the general features of synchronization, attractor fission,
and attractor fusion processes. The common characteristics shared by different
clusters in the segregation process are found. The effect of multiple different
time delays on synchronization is also investigated.
78. K.
Otsuka, M. Georgiou, and P. Mandel
"Intensity
Fluctuations In Multimode Lasers With Spatial Hole Burning"
Jpn.
J. Appl. Phys. Part 2 - Lett. 31 (9A), L1250-L1252 (1992).
ABSTRACT: The
intensity fluctuations in multimode lasers with spatial hole burning are
investigated. We give experimental evidence for a self-organized collective
behavior resulting from the cross saturation dynamics of spatially hole-burned
lasers, in which each mode is characterized by N relaxation oscillation
frequencies omega(l) (l = 1, 2, 3., N; N: number of oscillating modes), while
the total output exhibits a unique relaxation oscillation at the highest
frequency in omega(l) which coincides with that in a single mode laser.
79. K.
Otsuka, P. Mandel, S. Bielawski, D. Derozier, and P. Glorieux
"Alternate
Time Scale In Multimode Lasers"
Phys.
Rev. A 46 (3), 1692-1695 (1992).
ABSTRACT: We
analyze the intensity fluctuation of multimode lasers by extending the
linear-response theory of McCumber for single-mode lasers. In the two-mode
case, we prove analytically that the rate equations allow for an additional
dynamical oscillation frequency associated with the antiphase motion. This
explains the self-organized collective behavior of two-mode lasers, i.e., that
the total output behaves just like a single-mode laser. The linear stability
predicts the scaling law for this time scale, which results quite generally
through cross-saturation dynamics of population inversion. Experimental results
in two different laser systems confirm these predictions.
80. J. R.
Phillips, K. Tsubaki, T. Saku, and S. Tarucha
"Low-Frequency
Noise In Very High Mobility Modulation-Doped Structures"
Appl.
Phys. Lett. 61 (24), 2926-2928 (1992).
ABSTRACT: We
report here on the observation of low-frequency (1-100 Hz) noise characteristics
as a function of current in very high mobility four-terminal structures at 4.2
K. At low currents, the noise levels are too low to be observed with our
measurement system. When the mobility is decreased by a change in gate voltage,
or when the injected current is increased, noise levels increased. At currents
where excess noise is observable, the channel current-voltage characteristics
are nonlinear and the noise current dependence is superquadratic. The steep
current-dependence results from the degradation of mobility due to electron
heating, with the subsequent rapid noise increase due to optical phonon
scattering.
81. T. S.
Rao, Y. Horikoshi, C. Jagadish, R. G. Elliman, and J. S. Williams
"Characterization
Of Gaas/Si/Gaas Heterostructures"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 31
(10), 3282-3286 (1992).
ABSTRACT:
GaAs/Si(n)/GaAs, n = 1 to 3 mono-layers (ML) were grown on GaAs (100)
substrates using molecular beam epitaxy. Double crystal X-ray diffraction
rocking curve and Rutherford backscattering/chanelling studies indicated that 1
ML of Si grows coherently and psuedomorphicatly on GaAs and 2 and 3 ML Si
exhibit increasing defect nature and are probably relaxed. Raman scattering
measurements of the cap GaAs layer showed an increase in intensity of forbidden
transverse optical (TO) phonon peak with increasing underlying Si layer
thickness. Cross-sectional transmission electron microscopy studies revealed
that for 1 ML Si, the Si-GaAs interface and the Si layer are defect free.
However, for increasing thickness of Si to n = 2 and 3 ML, defect density
increased at the Si-GaAs cap layer interface.
82. T. S.
Rao, K. Nozawa, and Y. Horikoshi
"Growth
Of Gaas On Hydrogen-Fluoride Treated Si (100) Surfaces Using Migration-Enhanced
Epitaxy"
Appl.
Phys. Lett. 60 (13), 1606-1608 (1992).
ABSTRACT:
Heteroepitaxial growth of GaAs has been successfully achieved for the first
time using migration-enhanced epitaxy (300-degrees-C) on HF treated Si
substrates which have been subjected to an initial in situ pre-heat treatment
in the range of 350-620-degrees-C and without the customary high-temperature Si
oxide desorption step. High quality GaAs on Si exhibiting double-crystal x-ray
rocking curve full-width at half-maximum value of 280 arcsec was obtained by
using two-step growth technique MEE(300-degrees-C)/MBE (580-degrees-C).
Secondary-ion mass spectrometry studies indicated 0.05 (monolayer) ML of oxygen
at the interface of GaAs and HF treated Si substrate. The photoluminescene spectra
at 10 K for GaAs grown on HF treated Si substrates was dominated by sharp
excitonic related peaks and no carbon acceptor related emission could be
detected.
83. H. P. C.
Robinson, K. Torimitsu, Y. Kuroda, and A. Kawana
"Characterization
Of Spontaneous Synchronized Calcium Transients In Cultured Networks Of Cerebral
Cortical-Neurons"
Faseb
J. 6 (1), A511-A511 (1992).
ABSTRACT:
84. N.
Sarukura and Y. Ishida
"Ultrashort
Pulse Generation From A Passively Mode-Locked Ti-Sapphire Laser Based
System"
IEEE
J. Quantum Electron. 28 (10), 2134-2141 (1992).
ABSTRACT: The
detailed characteristics of a passively mode-locked Ti:sapphire laser using
saturable absorbers are described. This laser can stably generate nearly
transform-limited sub-100-fs pulses around 780 nm. Combining with this
oscillator and a double-pass Ti:sapphire amplifier pumped by a CW Q-switched
YAG laser (3 kHz) enables fiber-grating pulse compression down to 14 fs.
85. N.
Sarukura and Y. Ishida
"Pulse
Evolution Dynamics Of A Femtosecond Passively Mode-Locked Ti-Sapphire
Laser"
Opt.
Lett. 17 (1), 61-63 (1992).
ABSTRACT: The
pulse-formation process in a femtosecond passively mode-locked Ti:sapphire
laser with a saturable absorber is investigated. The time to reach the steady
state is approximately 200-mu-s. The formation time dependence on the dye
concentration and the coincidence of the steady-state pulse width with the
self-mode-locked state without a saturable absorber indicate that the function
of the saturable absorber is mainly to induce the initial modulation and to
shorten the pulse-formation time.
86. H. Sato,
M. Naito, T. Arima, and Y. Tokura
"La2-Xsrxcuo4(110)
Thin-Films Epitaxially Grown Along The Cuo2 Plane On Pr2cuo4
Single-Crystals"
Appl.
Phys. Lett. 61 (20), 2470-2472 (1992).
ABSTRACT: The
epitaxial growth of superconducting copper oxide films on nondoped insulating
copper oxide single crystals produced high-quality epitaxy perpendicular to the
c axis, namely along the CuO2 plane. The (110) oriented La1.84Sr0.16CuO4 (LSCO)
thin films with T(c) = 21 K were successfully grown on (110) Pr2CuO4
single-crystal substrates using 90-degrees off-axis sputtering. The x-ray
diffraction and the anisotropic resistivity indicate perfect in-plane epitaxy.
Scanning electron microscopy (SEM) shows fairly smooth surface of the (110)
LSCO film.
87. M. Sato
and Y. Horikoshi
"Effect
Of Indium Replacement By Gallium On Inas/Gaas Quantized Levels"
Surf.
Sci. 267 (1-3), 195-198 (1992).
ABSTRACT:
Quantized levels of InAs/GaAs thin layer structures are calculated using a
modified finite square well model, which takes into account In-Ga replacement
during growth. Comparison between the calculated results and experimental band
gaps indicates that In-Ga replacement rarely occurs in flow-rate modulation
epitaxy and that, in contrast, about 90% of the surface In is replaced by Ga in
molecular beam epitaxy. The effect of the replacement on the modulation of
GaAs/AlGaAs quantized levels by InAs layer insertion is also demonstrated.
88. S. C.
Shi, S. Ando, and T. Fukui
"Fabrication
Of High-Density Ultrafine Gaas Quantum Wire Array Structures Using Selective
Metalorganic Chemical Vapor-Deposition"
Surf.
Sci. 267 (1-3), 214-217 (1992).
ABSTRACT:
High density GaAs quantum wire array structures have been successfully
fabricated on an extremely short-period pattern. The quantum wire arrays were
formed on the sidewall gratings of a rectangular AlGaAs/GaAs multilayer
structure, selectively grown on a SiO2 masking (111)B substrate. The quantum
wires with the dimension of 25 x 35 nm2 had a period as small as 95 nm. The
fabrication process involved only selective metalorganic chemical vapor
deposition and a selective etching technique. No nanolithography patterning
techniques were used. The detailed fabrication process is presented.
89. N.
Shigekawa and E. Yamaguchi
"Effects
Of Disorder On Electronic Conduction Properties At Subsidiary Energy Minima In
Ternary Ingaas Alloys"
Semicond.
Sci. Technol. 7 (3B), B369-B371 (1992).
ABSTRACT: The
effects of disorder on the electronic conduction properties at subsidiary
energy minima (upper valleys) of In0.53Ga0.47As alloys are evaluated using a
novel Monte Carlo supercell approach with both the band-length and bond-angle
fluctuations considered. It is found that the width of the spectral function
obtained in the present approach is much larger than that obtained using the
coherent-potential approximation (CPA). This result indicates that the
bond-length and the bond-angle fluctuations-which are not sufficiently
considered in the CPA framework-induce strong effects on the electronic
properties of the upper valleys.
90. A.
Shimizu, T. Ogawa, and H. Sakaki
"2-Photon
Absorption-Spectra Of Quasi-Low-Dimensional Exciton Systems"
Phys.
Rev. B 45 (19), 11338-11341 (1992).
ABSTRACT: We
present a unified theory for two-photon absorption (TPA) spectra of Wannier
excitons in a low-dimensional semiconductor of an arbitrary dimension d = 0, 1,
2, and 3. It is found that the spectra strongly reflect the anisotropies of
both the band structure and the quasi-d-dimensional exciton envelope functions.
Therefore the low dimensionality can be sensitively detected by the TPA
spectroscopy. This is in striking contrast to the one-photon absorption
spectra, anisotropies of which cannot be taken as evidence of quantum
confinements.
91. A.
Shimizu, T. Ogawa, and H. Sakaki
"2-Photon
Absorption-Spectra Of Low-Dimensional Semiconductors"
Surf.
Sci. 263 (1-3), 512-517 (1992).
ABSTRACT: We
present a unified theory of two-photon absorption spectra of low-dimensional
semiconductors of an arbitrary dimension d = 0, 1, 2, 3. Widths of confining
potentials are assumed to be smaller than the exciton Bohr radius, and the
quasi-d-dimensional excitons play crucial roles in determining the spectra.
When d = 1 and 2, the spectra strongly depend on the polarization direction of
the incident light beam. This anisotropy comes from both anisotropies of the
exciton envelope functions and anisotropic band structure. This is in striking
contrast to one-photon absorption.
92. A.
Shimizu and M. Ueda
"Effects
Of Dephasing And Dissipation On Quantum Noise In Conductors"
Phys.
Rev. Lett. 69 (9), 1403-1406 (1992).
ABSTRACT: We
consider the nonequilibrium quantum noise of electrical current in
one-dimensional conductors, and clarify the mechanism that distinguishes
macroscopic conductors from mesoscopic conductors. The noise does not become of
the macroscopic type even when a strong dephasing is introduced. Macroscopic
noise is obtained only when the energy of the total electron system is
maximally dissipated when each electron traverses the conductor. Energy
transfer from the electron system to other systems is therefore essential for
noise suppression and for the noise to be macroscopic.
93. A.
Shimizu, M. Ueda, and H. Sakaki
"Quantum
Noises In Mesoscopic Conductors - Origins And Suppression"
Inst.
Phys. Conf. Ser. (127), 29-32 (1992).
ABSTRACT: It
is pointed out that the excess noise of mesoscopic conductors found by Lesovik
is the usual granularity noise, which is a general noise of quantum mechanics.
It is also shown that neither the dephasing nor the electron-electron inelastic
scattering is sufficient to suppress the excess noise. The excess noise is suppressed
and the noise characteristics becomes those of macroscopic conductors only when
the transit time of an electron across the conductor exceeds the energy
relaxation time due to the electron-phonon scatterings.
94. Y.
Shinoda, N. Shimizu, H. Hibino, T. Nishioka, C. Heimlich, Y. Kobayashi, S.
Ishizawa, K. Sugii, and M. Seki
"Surface
Structural-Changes During The Initial Growth Of Ge On Si(111)7 X 7"
Appl.
Surf. Sci. 60-1, 112-119 (1992).
ABSTRACT:
Reconstruction and the surface morphology of Ge layers on Si(111)7 x 7 during
the initial growth stages were studied by reflection high-energy electron
diffraction (RHEED) and transmission electron microscopy (TEM). The behavior of
the Ge layer subjected to a thermal process was clarified by solid-phase epitaxy
(SPE). By systematically varying the deposition thickness and temperature, the
growth mode was confirmed to be the Stranski-Krastanov mode and the
three-dimensional islands were found to form at 6.5 angstrom (equivalent to 4
ML). The 5 x 5 reconstructed structure was found to be characteristic of the
low coverage (below the critical thickness) and high-temperature annealing
(450-650-degrees-C). The double-step SPE, i.e., 5 angstrom Ge deposition (below
the critical thickness) followed by 2 angstrom Ge deposition (over the critical
thickness), revealed an apparent increase in the critical thickness. The
results show that the 5 x 5 reconstructed structure is derived from intermixing
Ge into the Si substrate.
95. H.
Shinojima, J. Yumoto, and N. Uesugi
"Size
Dependence Of Optical Nonlinearity Of Cdsse Microcrystallites Doped In
Glass"
Appl.
Phys. Lett. 60 (3), 298-300 (1992).
ABSTRACT:
This paper investigates the size dependence of the effective nonlinear cross
section sigma(eff) and the carrier recombination time on the size of
CdS0.12Se0.88 microcrystallites with average radii of 10, 30, 50, and 100
angstrom by degenerate four-wave mixing (DFWM) experiments. The decay curves of
the DFWM signal as a function of the probe delay time have fast and slow components.
As the microcrystallite size decreases, the fast component becomes dominant and
a carrier recombination time of 2 ps was observed in the 10-angstrom
microcrystallites. The diffraction efficiency of DFWM is almost the same for
all microcrystallites, that is, sigma(eff) has a weak size dependence. Smaller
microcrystallites show smaller magnitudes of the third-order nonlinear
susceptibility \chi(3)\, which is calculated from the measured effective
nonlinear cross section and the carrier recombination time.
96. K.
Shiraishi
"1st-Principles
Calculation Of The Migration Energy Of A Ga Adatom On An As-Stabilized
Gaas(001) Surface"
Appl.
Surf. Sci. 60-1, 210-214 (1992).
ABSTRACT: We
investigated the microscopic processes of a Ga adatom migration on an
As-stabilized GaAs(001) surface. The adiabatic potential surface of a Ga adatom
migration was calculated by the first-principles pseudopotential method on the
basis of local density functional formalism. We found that the most stable Ga
adsorption site is on the missing As dimer row and that the most favorable
migration pass is in the [110BAR] direction through the missing As dimer row.
The calculated activation barriers of a Ga adatom migration were 0.2 and 0.6 eV
in the [110BAR] and [110] directions, respectively.
97. K.
Shiraishi
"Ga
Adatom Diffusion On An As-Stabilized Gaas(001) Surface Via Missing As Dimer
Rows - 1st-Principles Calculation"
Appl.
Phys. Lett. 60 (11), 1363-1365 (1992).
ABSTRACT: We
have investigated the microscopic processes of Ga adatom diffusions on an
As-stabilized GaAs(001) surface by the first-principles pseudopotential method.
The results show that Ga adatoms diffuse on the surface by passing through the
missing As dimer rows. Comparison with the results of scanning tunneling
microscopy (STM) experiments during molecular beam epitaxy (MBE) growth
suggests that low As pressure increases the surface Ga adatom diffusion by a
formation of the continuous Ga adatom diffusion path. This is consistent with
the fact that low temperature growth is possible by migration enhanced epitaxy
(MEE), in which As and Ga sources are supplied alternately.
98. M. P.
Stopa
"Self-Consistent
Electronic-Structure And Optical Selection-Rules For Tetrahedral Quantum
Dots"
Surf.
Sci. 267 (1-3), 286-290 (1992).
ABSTRACT:
Recently, Fukui et al. (22nd conference on solid state devices and materials,
1990, Japan) have employed a controlled faceting technique in metal organic
chemical vapor deposition (MOCVD) crystal growth to construct tetrahedral
quantum dots without resorting to ion-implantation or chemical-etching
techniques. We investigate the electronic structure of these dots, in the
two-dimensional flat triangular approximation, with Hartree and exchange-correlation
interactions between electrons taken into account. We compute the
self-consistent electronic structure of a triangular dot in a density
functional formalism, taking into account finite barrier height and treating
exchange and correlation in the local density approximation. We present the
results of eigenvalues and density profiles as a function of charge number N,
dot size, and (perpendicular) magnetic field strength. We show that the
three-fold symmetry of the dot implies a form of the Bloch theorem that
separates the eigenfunctions into 'zones'. This allows us further to derive
selection rules for long-wavelength electromagnetic waves polarized arbitrarily
within the plane of the dot. These selection rules are independent of
self-consistent effects.
99. M. P.
Stopa
"Charging
Energy And Collective Response Of A Quantum Dot Resonant Tunneling Device"
Surf.
Sci. 263 (1-3), 433-437 (1992).
ABSTRACT:
Recent self-consistent electronic structure calculations and linear response
calculations of the current have sought to clarify the role of Coulomb charging
of a flat quantum dot connected via tunneling barriers to a two-dimensional
electron gas collector and emitter. In particular, resonant tunneling through
such a structure, which is observed to be periodic in a gate voltage applied to
the dot, is currently explained in terms of resonant suppression of the Coulomb
blockade by the gate. Nonetheless questions remain regarding the off resonance
activation energy and the possible role of collective excitations of the dot.
We calculate the self-consistent electronic structure of a two-dimensional
quantum dot connected via point-contact tunneling barriers to two wide 2DEG
regions, in the Hartree approximation. We include the effect of finite source-drain
voltage and side-gate voltages. We compute the charging energy for a single
electron entering the dot and discuss the dot capacitance. Finally, we compute
the approximate collective resonance frequency for charge oscillations in the
dot and discuss the possibility of plasmon coupling to single-electron
tunneling.
100. K. Sugii, S. Ishizawa, Y.
Kobayashi, H. Hibino, and M. Seki
"Tem
Moire Pattern And Scanning Auger-Electron Microscope Analysis Of Anomalous Si
Incorporation Into Mbe-Grown Ge On Si(111)"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 31
(10), 3296-3300 (1992).
ABSTRACT: Ge
islands are grown by molecular beam epitaxy (MBE) on Si(111) surfaces with an
SPE-grown buffer layer, which was expected to prevent intermixing between the
epitaxial Ge layer and the Si substrate. The epilayer composition analyzed from
the spacing of the Moire fringe indicates that the Ge islands should be a Si-Ge
alloy rather than pure Ge and that the alloying of Ge with Si is greater near
the edges of the island. The alloying phenomenon was verified by the
compositional depth profile analysis using the scanning Auger electron
microscope (SAM) technique. The Si incorporation into the Ge islands observed
here cannot be explained by a bulk diffusion mechanism and is a seriously
anomalous phenomenon since Si diffusion into Ge would be negligible at the growth
temperature and time used ill this experiment.
101. K. Sugiyama, O. Kondo, F.
Tomiyama, M. Date, Y. Hidaka, T. Ishii, and A. Matsuda
"Magnetizations
Of R2cuo4(R=Nd,Pr,Gd) Single-Crystals"
J.
Magn. Magn. Mater. 104, 1223-1224 (1992).
ABSTRACT: High-field
magnetizations of R2CuO4 (R = Nd, Pr and Gd) single crystals are investigated
up to 36 T at low temperatures. Nd2CuO4 shows two anomalous phase transitions
at 2.2 and 4.2 T along the [100] direction. The keyword to solve these
transitions is the staggered field due to the Cu spin. Pr2CuO4 shows weak
linear magnetization reflecting the singlet ground state of the Pr ion. Gd2CuO4
shows an anomalous but systematic multistep magnetization with a magnitude of
each step of about 10(-3)-mu-B per Gd ion in the c-plane beside the typical
antiferromagnetic magnetization with small anisotropy. The origin is not clear.
102. D. Sun and Y. Yamamoto
"Passive
Stabilization Of A Synchronously Pumped External-Cavity Surface-Emitting
Ingaas/Inp Multiple Quantum-Well Laser By A Coherent Photon-Seeding
Technique"
Appl.
Phys. Lett. 60 (11), 1286-1288 (1992).
ABSTRACT: A
synchronously pumped external-cavity surface-emitting InGaAs/InP multiple
quantum well laser was passively stabilized by a coherent photon-seeding technique
using an integrated output-coupling mirror. Both pulse duration and spectral
width were reduced significantly and the time-bandwidth product was reduced by
a factor of 30 to a near transform-limited value.
103. D. C. Sun, S. R. Friberg,
K. Watanabe, S. Machida, Y. Horikoshi, and Y. Yamamoto
"High-Power
And High-Efficiency Vertical Cavity Surface Emitting Gaas-Laser"
Appl.
Phys. Lett. 61 (13), 1502-1503 (1992).
ABSTRACT: We
report high power and high efficiency operation of a vertical cavity surface
emitting GaAs laser in an external cavity. The maximum cw output power from the
fundamental TEM00 mode was 700 mW at a temperature of 77 K when pumped by a cw
krypton-ion laser with 1.8 W pump power. We obtained an absolute quantum
efficiency (pump photons to lasing photons) of 44%, and a differential
efficiency above threshold of 58%.
104. M. Suzuki and T. Fukuda
"Observation
Of Indium On Gaas(110) Surfaces By Scanning Tunneling Microscopy"
Ultramicroscopy 42,
858-863 (1992).
ABSTRACT: The
surface structure of indium overlayers on cleaved p-type GaAs(110) is studied
by scanning tunneling microscopy in ultrahigh vacuum. About 1 monolayer of
indium was deposited on the surfaces at room temperature. We observed two types
of indium adsorption. One is linear clusters along the [110BAR] direction with
corrugation amplitudes 1-2 angstrom above the GaAs surface. The other type, in
which the second-layer indium atoms adsorb on the four-fold hollow site of the
first-layer indium atoms, is also obtained near the linear islands. It is found
that an In atom favors a Ga site rather than an As site for both types of
adsorption.
105. H. Tabei, T. Horiuchi, O.
Niwa, and M. Morita
"Highly
Sensitive Detection Of Reversible Species By Self-Induced Redox Cycling"
J.
Electroanal. Chem. 326 (1-2), 339-343 (1992).
ABSTRACT:
106. H. Tabei, M. Morita, O.
Niwa, and T. Horiuchi
"Fabrication
And Electrochemical Features Of New Carbon Based Interdigitated Array
Microelectrodes"
J.
Electroanal. Chem. 334 (1-2), 25-33 (1992).
ABSTRACT: A
new type of interdigitated array (IDA) microelectrode based on carbon film was
developed. A conductive carbon film was prepared on a platinum coated Si wafer
by the pyrolysis of 3,4,9,10-perylenetetracarboxylic dianhydride. The IDA
microelectrode was fabricated by photolithographic techniques from the
carbon/platinum composite film. The IDA electrode had 50 microband pairs. The
width of each microband was 3-mu-m with a length of 2 mm, and the gap between
two electrode bands was 2-mu-m. The electrode was characterized by cyclic
voltammetry with water soluble ferrocene and ruthenium hexa-amine. The
potential window without redox species was found to be similar to that of a
conventional glassy carbon electrode. The IR drop was negligible in a
measurement with 10-mu-M water soluble ferrocene at a moderate scan rate.
Generation-collection voltammograms of water soluble ferrocene and ruthenium
hexa-amine show clear limiting currents and their response in the negative
potential range was superior to that of conventional metal film IDA electrodes.
107. A. Taguchi, M. Taniguchi,
and K. Takahei
"Direct
Verification Of Energy Back Transfer From Yb 4f-Shell To Inp Host"
Appl.
Phys. Lett. 60 (8), 965-967 (1992).
ABSTRACT: We
report direct verification of energy back transfer from a Yb 4f-shell to an InP
host, which has been proposed as a quenching mechanism for the intrinsic
thermal quenching of intra-4f-shell luminescence. Photoluminescence time decay
of the band-edge related luminescence for a Yb-doped InP sample was examined.
In the temperature region from 100 to 120 K, it was observed that the
luminescence time-decay curve is composed of two exponential decay components.
The decay-time constant of the slower component in the band-edge related
luminescence is the same as that in the Yb 4f-shell luminescence. This fact
clearly shows that there is an energy transfer between the Yb 4f-shell
electronic state and the InP host electronic state, and the energy
back-transfer mechanism is the cause of the intrinsic thermal quenching of the
Yb intra-4f-shell luminescence.
108. T. Takagahara
"Quantum
Dot Lattice And Enhanced Excitonic Optical Nonlinearity"
Surf.
Sci. 267 (1-3), 310-314 (1992).
ABSTRACT: We
propose a concept of quantum dot lattice for enhancing the excitonic optical
nonlinearity, especially its figures of merit. The most important aspect of the
quantum dot lattice for enhancing the optical nonlinearity is the enlarged
exciton coherence length due to the cooperation of a large number of quantum
dots. The optical nonlinearity of the quantum dot lattice composed of typical
semiconductor materials is estimated and an enhancement in the figures of merit
of several orders of magnitude over the ever known values is predicted.
109. T. Takagahara and K.
Takeda
"Theory
Of The Quantum Confinement Effect On Excitons In Quantum Dots Of Indirect-Gap
Materials"
Phys.
Rev. B 46 (23), 15578-15581 (1992).
ABSTRACT: The
quantum confinement effect on excitons in quantum dots of indirect-pp materials
is investigated and a mechanism that induces an indirect-to-direct conversion
of the character of the optical transition is clarified. The exciton transition
energy and the exciton binding energy are calculated and found to be in good
agreement with experimental results on Si and Ge nanostructures. The large
exciton binding energy in Si and Ge quantum dots suggests that the
photoluminescence from these nanostructures is of excitonic origin even at room
temperature. The estimated radiative lifetime of excitons is strongly size
dependent and varies from nanosecond to millisecond corresponding to the
diameter from approximately 10 to approximately 30 angstrom. These theoretical
results suggest strongly the importance of the quantum confinement effect in the
luminescence processes of porous Si.
110. S. Takagi, M. Kimura, and
M. Katsuki
"A
Rapid And Efficient Protocol Of The Inverted Pcr Using 2 Primer Pairs"
Biotechniques 13
(2), 176-178 (1992).
ABSTRACT:
111. M. Takahashi, M. Morita,
O. Niwa, and H. Tabei
"Highly
Sensitive High-Performance Liquid-Chromatography Detection Of Catecholamine
With Interdigitated Array Microelectrodes"
J.
Electroanal. Chem. 335 (1-2), 253-263 (1992).
ABSTRACT:
Interdigitated array (IDA) microelectrodes in which both the band width and gap
are 2 mum were fabricated and applied to the electrochemical detectors used in
flow injection analysis (FIA) and high-performance liquid chromatography
(HPLC). The steady-state limiting current measured by FIA consists of the
one-third power flow dependent current and the flow independent current. This
flow independent current is caused by redox cycling. When an IDA electrode is
used, the current density is about ten times greater than with an ordinary
glassy carbon disk electrode. The high current density and low background noise
allowed the detection of 100 pM (2 fmol) of dopamine by HPLC measurement. It
was found that the peak current and sample concentration had a linear
relationship over a wide range (from 100 pM to 10 muM).
112. K. Takahei and H. Nakagome
"Photoluminescence
Characterization Of Nd-Doped Gap Grown By Metalorganic Chemical
Vapor-Deposition"
J.
Appl. Phys. 72 (8), 3674-3680 (1992).
ABSTRACT:
Nd-doped GaP is grown by metalorganic chemical vapor deposition and
characterized by photoluminescence measurements. The liquid-helium-temperature
luminescence spectra due to Nd intra-4f-shell transitions depend on the growth
conditions of the crystals. Some crystals show only a small number of
luminescence lines, while some other crystals show many luminescence lines,
indicating the presence of many kinds of Nd light emitting centers. Intensities
of some luminescence lines begin to decrease at about 50 K and they are below
the detection limit at 100 K. However, thermal quenching of some other
luminescence lines begins at higher temperatures and their luminescence can be
observed up to room temperature. A study on photoexcitation with above and
below-band gap energy photons reveals that some Nd centers can be excited even
by below-band gap energy photons, indicating the role of mid-pp levels, in the
excitation mechanism, related to the Nd centers. A further comparative study of
luminescence characteristics on GaP and GaAs doped with Nd shows that the
experimental evidence is consistent with the excitation mechanism proposed for
intra-4f-shell luminescence of Yb in InP, where the rare earth 4f shells are
excited by way of electron-hole recombination at rare-earth-related trap levels
with successive energy transfer.
113. K. Takeda and K. Shiraishi
"Electronic-Structure
Of Chain-Like Polystannane"
Chem.
Phys. Lett. 195 (2-3), 121-126 (1992).
ABSTRACT: The
electronic structure of polystannane (PSn), (SnH2)n, has been calculated by the
first principle local density functional method. The effect of bond-angle
distortion on PSn's first band gap is also investigated theoretically. The
common features in the group IV polymers are then summarized by comparison with
previous calculated results for polysilane (SiH2)n and polygermane (GeH2)n.
114. K. Takeda and K. Shiraishi
"1st-Principles
Calculations On Adiabatic Potential Surfaces Of Hydrogen-Atoms In
Polysilane"
Philos.
Mag. B-Phys. Condens. Matter Stat. Mech. Electron. Opt. Magn. Prop. 65
(3), 535-552 (1992).
ABSTRACT:
Adiabatic potential surfaces are calculated for an H atom at various positions
in polysilane. The calculations are based on local-density-functional theory,
using pseudo-potentials, in a supercell geometry. The migration paths for a H
atom dissociated from the side-chain position, and for a foreign H atom are
investigated. One possible path entwines the Si skeleton. Bond switching due to
breaking the Si-H bond and the ensuing H migration is also discussed on the
basis of three hypothetical atomic configurations.
115. K. Takei and Y. Maeda
"Nmr-Study
On Compositional Distribution In Sputter-Deposited Co-Ni Thin-Films"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 31
(9A), 2734-2735 (1992).
ABSTRACT:
Compositional distribution in sputter-deposited Co-Ni films was measured by
using spin echo Co-59 NMR. The NMR frequency spectra of Co-Ni films were very
similar to those of compositionally homogeneous Co-Ni powdered alloys. A simulation
of the NMR spectra indicated that the Co-Ni films were in a compositionally
homogeneous state in which the Co and Ni were distributed randomly at the
lattice sites.
116. M. Taniguchi, H. Nakagome,
and K. Takahei
"Luminescence
Lifetime Studies Of Nd-Doped Gap And Gaas"
J.
Lumines. 52 (5-6), 251-257 (1992).
ABSTRACT:
Photoluminescence time decay experiments are performed for the first time at
liquid helium temperature on Nd-doped GaP samples which show sharply structured
(1-mu-m) luminescence spectra due to Nd-intra-4f-shell transitions. It is found
that the luminescence lifetimes are different for luminesence lines originating
from different Nd centers. The observed 4 K lifetimes (16-20-mu-s) are longer
than the 77 K lifetime (5-mu-s) previously observed from an ion-implanted
GaP:Nd sample. The temperature dependence of the luminescence lifetime is also
reported. A similar lifetime value of 12-mu-s is observed from a GaAs: Nd
sample at 4 K. These intrinsic 4 K lifetimes of Nd in GaP and GaAs are shorter
than the lifetimes of Nd in II-VI compounds and ionic crystals. It is probably
due to the stronger covalent bonding between Nd ions and the host crystals or
the lower symmetry of Nd sites in GaP and GaAs hosts.
117. S. Tarucha, Y. K. Fukai,
Y. Hirayama, and T. Saku
"Ballistic
Electron Propagation In Macroscopic 4-Terminal Structures And Its Gate
Controlled Transmission And Reflection"
Surf.
Sci. 263 (1-3), 253-257 (1992).
ABSTRACT:
Ballistic electron transport in macroscopic four-terminal devices with a high
electron mobility is studied. The bend resistance characteristics are well
analyzed using the Landauer-Buttiker formula although the leads are too wide to
form well-defined one-dimensional subbands. The ballistic length determined
from this analysis agrees well with the mean free path deduced from a mobility
and electron density. Transmission and reflection of ballistic electrons are
manipulated using a strip gate placed so as to bisect the device. The
transmission and reflection probabilities are determined as a function of gate
voltage, and related to the change in the refraction of ballistic electron
propagation across the regions of different electron densities.
118. S. Tarucha, T. Saku, Y.
Hirayama, and Y. Horikoshi
"Bend-Resistance
Characteristics Of Macroscopic 4-Terminal Devices With A High
Electron-Mobility"
Phys.
Rev. B 45 (23), 13465-13468 (1992).
ABSTRACT:
Bend-resistance characteristics are studied for four-terminal ballistic devices
with a high electron mobility on a macroscopic scale of order 10-100-mu-m. The
negative bend resistance induced by ballistic electron transport is
quantitatively reproduced by the Landauer-Buttiker formula in the classical
limit for various device sizes and electron densities. Using this formula, we
determine the ballistic electron length as a function of electron density,
which compares well with the elastic mean free path deduced from the electron
mobility and electron density.
119. S. Tarucha, T. Saku, Y.
Hirayama, J. R. Phillips, K. Tsubaki, and Y. Horikoshi
"Ballistic
Transport And Low-Frequency Noise In High-Mobility 2-Dimensional
Electron-Systems"
Inst.
Phys. Conf. Ser. (127), 127-132 (1992).
ABSTRACT:
Ballistic transport and low-frequency noise are studied for two-dimensional
electrons of very high electron mobility. Using macroscopic-scale devices, we
reveal two major properties of ballistic transport: long-distance ballistic
transport of electrons and size-independent resistance. These behaviors are
well reproduced by the Landauer-Buttiker formula in the classical limit. We
observe critical noise generation for a large injection current in a wide
channel device. This arises from nonequilibrium electron heating under high
electric field.
120. H. Teramae
"Electronic-Properties
Of Polymeric Silicon Hydrides - Comment"
Phys.
Rev. B 46 (19), 12788-12789 (1992).
ABSTRACT: The
electronic structure of the polysilene chain is studied by means of the ab
initio crystal orbital calculations. The electronic structure of polysilene is
not metallic at the Hartree-Fock level and the effect of the inclusion of the d
orbitals on silicon is small. These conclusions are completely different from
the recent work of Springborg.
121. Y. Tokura, T. Saku, S.
Tarucha, and Y. Horikoshi
"Anisotropic
Roughness Scattering At A Heterostructure Interface"
Phys.
Rev. B 46 (23), 15558-15561 (1992).
ABSTRACT:
Anisotropic Hall mobilities of a two-dimensional electron gas are observed in
modulation-doped AlxGa1-xAs/GaAs heterostructures grown by molecular-beam
epitaxy on a (001) GaAs substrate. The mobility in the [110BAR] direction is
larger than that in the [110] direction. An anisotropic in roughness is
proposed to account for the observed anisotropic Hall mobilities.- The
dependences of the anisotropic mobilities on the electron concentration are
explained well by the theoretical calculation, which assumes the existence of
interface islands longer in the [110BAR] direction than in the [110] direction.
This assumption is consistent with previous reports on in situ measurement of
growing surfaces by scanning tunneling microscope and electron diffraction.
122. K. Tsubaki, T. Honda, H.
Saito, and T. Fukui
"Electron
Wave Interference In Fractional Layer Superlattice (Fls) Quantum Wires"
Inst.
Phys. Conf. Ser. (120), 619-624 (1992).
ABSTRACT:
123. K. Tsubaki, T. Honda, H.
Saito, and T. Fukui
"Density
Of States Of Alas/Gaas Fractional Layer Superlattice Quantum Wires In A
Modulation Doped Structure"
Surf.
Sci. 267 (1-3), 270-273 (1992).
ABSTRACT: The
density of states (DOS) of AlAs/GaAs fractional layer superlattice (FLS)
quantum wires is found to consist of one-dimensional and zero-dimensional
states. The FLS quantum wires are fabricated by electron beam lithography from
the AlAs/GaAs FLS modulation doped heterostructure. The periodicity of the FLS
quantum wires is 8 nm and the width is 0.25-mu-m. Drain current oscillations
with negative transconductance is observed below 7.5 K due to a reduction in
wire width. The density of states is estimated from the temperature dependence
of the threshold voltage (V(th)). Since the DOS of the FLS quantum wire
structure has sharper peaks than that of the unconfined FLS modulation-doped
structure, which has both one-dimensional and two-dimensional electron states,
we can conclude that the additional sub-micron confinement reduces these states
to zero-dimensional and one-dimensional, respectively.
124. K. Tsubaki, T. Honda, and
Y. Tokura
"Aharonov-Bohm
Effect Under High Magnetic-Field In A Corbino Disk Antidot Channel"
Surf.
Sci. 263 (1-3), 392-395 (1992).
ABSTRACT:
Corbino disk anti-dots are fabricated by distributing several thousand sub-mu-m
square holes throughout a square Corbino disk channel. The magnetoresistance
(magnetoconductance) or Corbino disk anti-dots up to 10 T displays a periodic
oscillation over the entire magnetic field at temperatures below 0.1 K. Since
Corbino disk anti-dots prevent electrons from flowing along an edge, electrons
go around the shallow etched holes under a high magnetic field. The periodic
oscillation comes from the Aharonov-Bohm (A-B) effect, which is the electron
wave interference of electron trajectories encircling the magnetic flux which
penetrates through the shallow-etched hole.
125. H. Tsubokawa, K. Oguro, H.
P. C. Robinson, T. Masuzawa, T. Kirino, and N. Kawai
"Abnormal
Ca2+ Homeostasis Before Cell-Death Revealed By Whole Cell Recording Of Ischemic
Ca1 Hippocampal-Neurons"
Neuroscience 49
(4), 807-817 (1992).
ABSTRACT:
Slices were made from the hippocampus of gerbils following transient ischemia
achieved by clamping the carotid arteries for 5 min, and changes in the
electrophysiology of CA1 pyramidal neurons were studied by whole cell
patch-clamp recording as well as conventional intracellular recording. The
great majority of CA1 neurons in slices made 2.5-3 days after ischemia showed
reduced resting potentials and were easily depolarized by prolonged
low-frequency stimulation or by tetanic stimulation of the Schaffer
collateral/commissural input. This stimulus-induced depolarization was
accelerated by intracellular injection of D-Myo-inositol 1,4,5-triphosphate,
which depolarized membrane potentials towards 0 mV without synaptic input
stimulation. Intracellular application of BAPTA, a Ca2+ chelator, effectively
blocked the stimulus-induced depolarization. When recording from ischemic
neurons with patch pipettes containing both D-Myo-inositol 1,4,5-triphosphate
and BAPTA, excitatory postsynaptic currents were transiently potentiated by
stimulation, but the membrane potential did not show stimulus-induced
depolarization and remained steady for long periods. These results lend support
to the view that the intracellular Ca2+ regulation system is severely disturbed
following ischemia, and that input fiber stimulation leads to abnormal Ca2+
accumulation in ischemic neurons resulted in neuronal death. The reduction of
free Ca2+ inside the ischemic neuron by BAPTA apparently saves neurons which
are otherwise destined to delayed neuronal death.
126. M. Ueda, N. Imoto, H.
Nagaoka, and T. Ogawa
"Continuous
Quantum-Nondemolition Measurement Of Photon Number"
Phys.
Rev. A 46 (5), 2859-2869 (1992).
ABSTRACT:
This paper presents a general theory for a continuous quantum-nondemolition
measurement of photon number. This theory treats a time-distributed measurement
as a sequence of measurements in which at most one photon can be detected in an
infinitesimal time, and shows that the average number of photons remaining in
the measured field increases when a photon is detected and decreases when no
photon is detected. The state of the measured system evolves nonunitarily and
reduces continuously to a number state whose eigenvalue is uniquely determined
by the average rate of photodetection and whose probability distribution
coincides with the initial photon-number distribution. Applying the general
theory to typical quantum states - coherent, thermal, and squeezed states -
shows that the continuous-state reduction towards a number state depends
strongly on the initial photon statistics. Despite the nonunitarity of state
evolution, an initially pure state keeps its purity: the initial density
operator becomes diagonalized only if the readout information is discarded.
127. M. Ueda and M. Kitagawa
"Reversibility
In Quantum Measurement Processes"
Phys.
Rev. Lett. 68 (23), 3424-3427 (1992).
ABSTRACT: A
measurement process is logically reversible if the premeasurement density
operator of the measured system can be calculated from the postmeasurement
density operator and the readout of the measuring apparatus. We show that the
continuous-measurement version of a quantum counter, unlike the conventional
photon counter, performs a logically reversible measurement. The physical
origin for such a distinction is found to be sensitivity to vacuum field
fluctuations.
128. M. Ueda and S. Kurihara
"Infrared
Divergence In Single-Electron Tunneling"
Phys.
Rev. B 46 (19), 12568-12572 (1992).
ABSTRACT: In
small-capacitance normal tunnel junctions, even a single-electron tunneling
causes a substantial change in the localized Coulomb potential. If the
perturbation may be regarded as static, Fermi liquid theory requires that
infinitely many electron-hole pairs should be excited near the Fermi surface. It
is shown that such infrared divergence leads to a power-law anomaly in
tunneling conductance. Possible experimental situations to observe this effect
are discussed.
129. T. Wakahara, H. Murase,
and K. Odaka
"Online
Handwriting Recognition"
Proc.
IEEE 80 (7), 1181-1194 (1992).
ABSTRACT:
On-line handwriting recognition means that a machine recognizes each character
as it is being written. For large-alphabet languages, like Japanese,
handwriting input using an on-line recognition technique is essential for input
accuracy and speed. It offers several advantages over off-line handwriting
recognition. However, there are serious problems that prevent high recognition
accuracy without imposing handwriting constraints. First, the thousands of
ideographic Japanese characters of Chinese origin (called Kanji) can be written
with wide variations in the number and order of strokes and significant shape
distortions. Also, writing box-free recognition of characters is required to
create a better man-machine interface. This paper describes the intense research
performed by NTT over the past 15 years to answer the most pressing recognition
problems. Prototype systems developed by NTT are also described. Last, the
man-machine interfaces made possible with on-line handwriting recognition and
anticipated advances in both hardware and software are discussed.
130. M. Weyers, M. Sato, and H.
Ando
"Red
Shift Of Photoluminescence And Absorption In Dilute Gaasn Alloy Layers"
Jpn.
J. Appl. Phys. Part 2 - Lett. 31 (7A), L853-L855 (1992).
ABSTRACT: We
present the first report on the optical properties of dilute GaAS1-xNx alloys
(0<x<0.015). The layers have been grown by plasma-assisted metalorganic
chemical vapor deposition (MOCVD). The grown layers show a systematic red shift
of the band-edge luminescence with increasing N content. The assignement of the
phoyoluminescence to band-edge transitions and not to isolated N-N pair
emission is verified by the characteristics of the optical absorption.
131. M. Weyers and K. Shiraishi
"Carbon
In Iii-V Compounds - A Theoretical Approach"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 31
(8), 2483-2487 (1992).
ABSTRACT:
Carbon as a very well behaved acceptor dopant in GaAs/AlGaAs is already
successfully used in many device applications. However, the physics governing
its incorporation behavior (amphoteric impurity) into III-V semiconductors is
currently not well understood. We present a calculation from first principles
of the change in total energy accompanying the incorporation of carbon onto
lattice sites in the III-V compounds AIP, GaP, InP; and AlAs, Ga.As and InAs.
Taking into account the energy gained by filling a group III or group V vacancy
with carbon, the obtained p-type conduction in carbon doped GaAs, AlAs, GaP
(and presumably AlP) as well as the n-type conduction in InP can be explained
based on the results of our total energy calculations. Additionally, the
observed trends in the energy gain can explain the observed differences in
tendency for carbon incorporation into the compounds under study.
132. K. Winer
"Behavior
Of Excess As In Nonstoichiometric Si-Doped Gaas"
J.
Appl. Phys. 71 (12), 5841-5846 (1992).
ABSTRACT: The
Si doping efficiency (=[e-]/[Si]) in homoepitaxial GaAs has been measured as a
function of molecular beam epitaxial growth conditions (As pressure, substrate
temperature, and growth rate) and post-growth thermal annealing conditions. The
doping efficiency decreases from one under optimal growth conditions to almost
zero: (1) exponentially with inverse substrate temperature below 400-degrees-C
and (2) as a power law in the As4-to-Ga beam-equivalent fluence ratio above
unity. The doping efficiency of nonoptimally grown films increases from almost
zero to near one upon post-growth thermal annealing above 650-degrees-C with
slower than exponential kinetics. These changes are attributed to charge
trapping into and release from, respectively, excess-As-related defects, which
are incorporated during growth and removed by out-diffusion during annealing.
133. S. Yamada, H. Asai, and Y.
Kawamura
"Subband
Effective Mass And Mobility Of 2-Dimensional Electrons In Uniformly Si-Doped
Ga0.47in0.53as/Al0.48in0.52as Multiple Quantum-Wells"
J.
Appl. Phys. 72 (2), 569-574 (1992).
ABSTRACT:
Subband effective mass and mobility of a two-dimensional electron gas in
uniformly Si-doped Ga0.47In0.53As/Al0.48In0.52As multiple quantum wells are
estimated. In three samples with well widths of 130, 200, and 300 angstrom and
a fixed barrier width of 68 angstrom, up to three two-dimensional subbands are
found. Maximum enhancement of electron effective mass is 25% over the bulk
value at a Fermi energy of 108 meV. These estimated effective masses are
slightly smaller than previously reported values, and this is explained by
recent theories which assume only nonparabolic correction. When the temperature
ratio, (Dingle temperature)/(mobility temperature), is assumed to be identical
in different subbands in each sample, the electron mobility of the first
excited subband is at most twice that of the ground subband in the sample with
the widest well. The effects of intersubband scattering and of screening on the
subband mobilities are also discussed.
134. S. Yamada and M. Yamamoto
"Possible
Conductance Quantization In Narrow Wires With Point-Contact Boundaries"
Phys.
Rev. B 45 (24), 14162-14166 (1992).
ABSTRACT:
Longitudinal conductance in quasiballistic narrow wires reveals plateaus if the
wires have point-contact (PC) boundaries. When two PC boundaries defining a
quasiballistic wire are opposite each other and weakly coupled, the conductance
difference between the successive plateaus is almost constant under zero and
relatively low magnetic fields and the magnitude is likely DELTA-G
approximately f(c)(2e2/h), where f(c) is a constant less than 1. This value
changes, depending on the wire conductance and on the differences in electrical
characteristics between the two PC's. The origin of the appearance of the
plateaus is also discussed briefly.
135. S. Yamada and M. Yamamoto
"Direct
Estimation Of Quantized Thermopower In A Single Point Contact"
Semicond.
Sci. Technol. 7 (3B), B289-B291 (1992).
ABSTRACT: The
quantized thermopower in the ballistic regime was estimated directly from
measurements in a single point contact with a specific configuration of ohmic
electrodes. If the DC current supplied to heat electrons increased over a
critical value, increases of both the electron and lattice temperatures were
observed. For the lower indices of the one-dimensional subbands (i = 1 and 2),
the measured thermopower peak differed by as much as 20% from the theoretically
predicted value. At low currents, where only the electron temperature was
raised, the agreement with theory was within 10%.
136. S. Yamada, M. Yamamoto,
and K. Aihara
"Quantum
Oscillations Of Transverse Resistance In Series And Single Point-Contact
Configurations"
Surf.
Sci. 263 (1-3), 265-269 (1992).
ABSTRACT: We
report in this work quantum oscillations in transverse resistance in series and
single point-contact (PC) configurations. In the series case, both under zero
and finite magnetic fields, an oscillation corresponding to the plateaus of the
longitudinal resistance was observed. In the single PC with an accurate
structure symmetry, a similar oscillation appeared only when a finite magnetic
field was applied. In addition, it is confirmed that the oscillations occur at
equilibrium conditions and their polarity is odd against reversal of the
current direction. These results indicate a new and equilibrium origin of the
oscillation, which is different from the oscillatory thermopower.
137. H. Yamaguchi and Y.
Horikoshi
"As
Desorption From Gaas And Inas Surfaces Studied By Improved High-Energy Electron
Reflectivity Measurements"
Appl.
Surf. Sci. 60-1, 224-227 (1992).
ABSTRACT: The
electron beam specular reflectivity of GaAs and InAs (001) surfaces at several
temperatures was quantitatively evaluated by measuring the current through an
electrode in front of the fluorescence screen. At the reconstruction
transition, the reflectivity as a function of substrate temperature changes
discontinuously with a hysteresis cycle for InAs and changes continuously
without a hysteresis for GaAs. This difference indicates that the order of
surface structure transition differs between these two surfaces. The
reflectivity changes during As desorption show that the desorption process is
sensitive to surface structure transition and that the desorption at the
structure transition differs between different orders of surface structure
transitions.
138. H. Yamaguchi and Y.
Horikoshi
"Growth
Of Gaas/Eras/Gaas Structures By Migration-Enhanced Epitaxy"
Appl.
Phys. Lett. 60 (19), 2341-2343 (1992).
ABSTRACT:
Monocrystalline GaAs/ErAs/GaAs structures are fabricated by migration-enhanced
epitaxy at 320-degrees-C. When the ErAs layer thickness is less than 3
monolayers, reflection high-energy electron diffraction patterns, double
crystal x-ray diffraction analysis, and transmission electron microscopy
observations show successful overgrowth of GaAs on the ErAs layer. Distinct
satellite peaks are observed in an x-ray rocking curve of an ErAs/GaAs
superlattice grown under a similar condition, indicating that high-quality
multilayer structures with very thin ErAs layers can be fabricated by
migration-enhanced epitaxy.
139. H. Yamaguchi and Y.
Horikoshi
"As
Desorption From Gaas And Alas Surfaces Studied By Improved High-Energy Electron
Reflectivity Measurements"
J.
Appl. Phys. 71 (4), 1753-1759 (1992).
ABSTRACT: The
desorption of As from GaAs (001), (111)B, and AlAs(001) is studied in detail by
measuring the electron-beam current reflected from these surfaces. When the As
supply to the surface was terminated, the electron specular reflectivity
decreases exponentially with time due to the As desorption. The decay rate was
much smaller for AlAs (001) than for GaAs (001) and (111)B, which indicates
stronger atomic bonding for AlAs than for GaAs. For the GaAs (001) surface, the
decay rate and the activation energy for the decay in specular reflectivity
change discontinuously at the transition between (2 x 4) and (3 x 1)
reconstructions. This shows the As desorption process is sensitive to the
transition of surface reconstruction. The dependence of the As desorption rate
on the thickness of the top GaAs layer in GaAs/AlAs heterostructures indicates
an abrupt change of bond strength near the interface.
140. H. Yamaguchi and Y.
Horikoshi
"1st-Order
Surface-Structure Transition On The (001) Inas Surface Studied With Improved
High-Energy Electron Reflectivity Measurements"
Phys.
Rev. B 45 (3), 1511-1513 (1992).
ABSTRACT: The
electron-beam specular reflectivity of an InAs(001) surface was quantitatively
measured as current through an electrode at several substrate temperatures. The
reflectivity changes discontinuously at the reconstruction transition from
As-stable (2 x 4) to In-stable (4 x 2) with hysteresis cycle as a function of
the substrate temperature, indicating a first-order transition. The
reflectivity change during As desorption shows that the desorption rate has a
local minimum at the transition because of the existence of a metastable state
due to the first-order transition.
141. Y. Yamamoto and H. A. Haus
"Effect
Of Electrical Partition Noise On Squeezing In Semiconductor-Lasers"
Phys.
Rev. A 45 (9), 6596-6604 (1992).
ABSTRACT:
Amplitude fluctuations in the light from a laser and the partition noise
attributable to a beam splitter are analyzed using an equivalent-circuit model
that incorporates amplitude squeezing. When the energy is not carried by
photons but by electrons and also when electrons can be treated as classical
particles, the circuit model need not be changed. One simply applies the
general circuit model to low frequencies h-nu << k(B)T. Conversion of an
electric current to photon flux, and vice versa, converts classical
sub-shot-noise spectra of electric currents into quantum squeezing of photon
fluxes, and vice versa. The sub-shot-noise character of electric currents,
unlike that of quantum squeezing, is not necessarily destroyed by current loss.
142. Y. Yamamoto, S. Machida,
and G. Bjork
"Cavity
Quantum Electrodynamics In Quantum-Well Lasers"
Surf.
Sci. 267 (1-3), 605-611 (1992).
ABSTRACT: The
physics and applications of cavity quantum electrodynamics in semiconductor
lasers are discussed. Spontaneous emission from a quantum well was drastically
modified by the microcavity structure. The increase in the coupling efficiency
of spontaneous emission into a cavity resonant mode leads to the reduction of
the threshold current. Oscillation without inversion is possible if the
coupling efficiency is increased to close to one.
143. Y. Yamamoto, S. Machida,
and G. Bjork
"Micro-Cavity
Semiconductor-Lasers With Controlled Spontaneous Emission"
Opt.
Quantum Electron. 24 (2), S215-S243 (1992).
ABSTRACT: The
principle and applications of quantum electrodynamics in microcavity
semiconductor lasers are reviewed. The coupling efficiency of spontaneous
emission into a lasing mode and the spontaneous lifetime are modified by
various microcavity structures. As a consequence of the increased coupling
efficiency, those microcavity semiconductor lasers are expected to feature a
low threshold current, high quantum efficiency and broad modulation bandwidth.
One remarkable result of the increased coupling efficiency is 'lasing without inversion'.
The other is 'intensity squeezing at any pump rate'.
144. Y. Yamamoto, S. Machida,
and W. H. Richardson
"Photon
Number Squeezed States In Semiconductor-Lasers"
Science 255
(5049), 1219-1224 (1992).
ABSTRACT:
Electromagnetic fields, with the noise on one quadrature component reduced to
below the quantum mechanical zero-point fluctuation level and the noise on the
other quadrature component enhanced to above it, are currently of great
interest in quantum optics because of their potential applications to various
precision measurements. Such squeezed states of light are usually produced by
imposing nonlinear unitary evolution on coherent (or vacuum) states. On the
other hand, squeezed states with reduced photon number noise and enhanced phase
noise are generated directly by a constant current - driven semiconductor
laser. This is the simplest scheme for the generation of nonclassical light,
and so far it has yielded the largest quantum noise reduction. The mutual
coupling between a lasing junction and an external electrical circuit provides
opportunities for exploring the macroscopic and microscopic quantum effects in
open systems.
145. Y. Yamamoto and S. Tarucha
"Regulated
Single Electron To Single Photon Conversion In A Constant-Current-Driven Pn
Microjunction"
Jpn.
J. Appl. Phys. Part 2 - Lett. 31 (8B), L1198-L1201 (1992).
ABSTRACT: The
single electron-hole pair injection followed by the emission of a single photon
is regulated with time separation tau = e/I in a constant-current-driven
semiconductor pn microjunction. Oscillation of the junction voltage with a
frequency f = I/e results from the coexistence of continuous uniform charging
into a depletion layer via a high-impedance constant-current source and
discrete thermionic emission of an electron into the active p-region. The
principle is similar to the Coulomb blockade in an ultrasmall-capacitance
tunnel junction. The proposed scheme is expected to open up an interesting new
field of combined single electronics and single photonics.
146. Y. Yamauchi and N.
Kobayashi
"Decomposition
Process Of Alane And Gallane Compounds In Metal-Organic Chemical
Vapor-Deposition Studied By Surface Photoabsorption"
Jpn.
J. Appl. Phys. Part 2 - Lett. 31 (9A), L1263-L1265 (1992).
ABSTRACT: We
used surface photo-absorption (SPA) to study trimethylamine alane (TMAA) and
dimethylamine gallane (DMAG) decomposition processes on a substrate surface in
metal-organic chemical vapor deposition. The decomposition onset temperatures
of these group III hydride sources correspond to the substrate temperature at
which the SPA reflectivity starts to increase during the supply of the group
III source onto a group V stabilized surface. It was found that TMAA and DMAG
start to decompose at about 150-degrees-C on an As-stabilized surface, which is
much lower than the decomposition onsets of trialkyl Al and Ga compounds. Low
temperature photoluminescence spectra exhibit dominant excitionic emissions for
GaAs layers grown by DMAG at substrate temperatures above 400-degrees-C,
indicating that carbon incorporation and the crystal quality deterioration due
to incomplete decomposition on surface is much suppressed by using DMAG. A
comparison of AlGaAs photoluminescence between layers by TMAA/triethylgallium
and triethylaluminum/triethylgallium shows that the band-to-carbon acceptor
transition is greatly reduced by using TMAA. TMAA and DMAG were verified to be
promising group III sources for low-temperature and high-purity growth with
low-carbon incorporation.
147. T. Yanagawa, H. Nakano, Y.
Ishida, and Y. Sasaki
"Photodarkening
Mechanism In Colored Filter Glasses"
Opt.
Commun. 88 (4-6), 371-375 (1992).
ABSTRACT: It
is clearly shown that a nanosecond pulse dye laser can provide the same
photodarkening effect in colored filter glasses as a picosecond hybridly
mode-locked dye laser. This suggests that the photodarkening mechanism is
associated with a kind of solarization and a state of surface activation due to
the production of a snowball comprised of impurity ions around CdSxSe1-x
microcrystallites. It is also shown that the laser annealing effect is the same
as the photodarkening effect.
148. R. Yano, M. Mitsunaga, and
N. Uesugi
"Stimulated-Photon-Echo
Spectroscopy.1. Spectral Diffusion In Eu3+ Yalo3"
Phys.
Rev. B 45 (22), 12752-12759 (1992).
ABSTRACT:
Systematic measurements of stimulated-photon-echo intensities as a function of
the first-to-second (tau) and second-to-third (T) pulse separations allow the
investigation of the dynamical properties of the spectral diffusion for the
F-7(0)-D-5(0) transition of a cryogenic Eu3+:YAlO3 sample. The existence of
spectral diffusion was verified by the significant broadening (from 1.2 to 7.2
kHz) of the homogeneous linewidth (GAMMA) as T increases from microseconds to
milliseconds, the effect being attributed to the flip flop of nearby aluminum
nuclear spins surrounding the Eu3+ ion. A similar broadening effect (from 0.61
kHz, to a few kHz) was also observed in the presence of a static magnetic field
H0 = 137 G, but with a much slower diffusion rate. To explain these
observations, we use three theoretical models: the Bai-Fayer model, the
diffusion-equation model, and the Monte Carlo model. Each agrees reasonably
well with the experimental data and indicates the flip rates of sub-kHz order
at H0 = 0 and an order of magnitude lower at 137 G.
149. R. Yano, M. Mitsunaga, and
N. Uesugi
"Nonlinear
Laser Spectroscopy Of Eu3+Y2sio5 And Its Application To Time-Domain Optical
Memory"
J.
Opt. Soc. Am. B-Opt. Phys. 9 (6), 992-997 (1992).
ABSTRACT:
Linear- and nonlinear-optical properties of Eu3+:Y2SiO5 have been investigated.
All the energy levels of the 7F0,1,2. ground-state manifold and the 5D0,1,2
excited-state manifold were identified, and they were found to be doubly
structured because of the two inequivalent optical sites. Two absorption lines
of the 7F0-5D0 transition were studied in detail by using nonlinear
spectroscopic techniques, photon-echo and stimulated-photon-echo methods. It
was found by the photon-echo measurement that the optical dephasing time for
one site is extremely long and is excitation-intensity dependent. With the
smallest possible intensity we observed the longest ever dephasing time in a
solid, 822-mu-s, or a 387-Hz homogeneous linewidth. From the
stimulated-photon-echo measurement, the linewidth was found to be constant over
a wide range of time scales, implying the absence of spectral diffusion in this
crystal. These quite advantageous properties of this crystal were used for the
demonstration of two novel types of time-domain optical data readout: time- and
frequency-domain hybrid optical memory and spectrally programmed coherent
transients.
150. R. Yoshimura, H. Nakagome,
S. Imamura, and T. Izawa
"Coupling
Ratio Control Of Polymeric Wave-Guide Couplers By Bending"
Electron.
Lett. 28 (23), 2135-2136 (1992).
ABSTRACT:
Directional couplers are successfully fabricated on acrylic substrates using polymers
synthesised from deuterated methacrylate and deuterated fluoromethacrylate
monomers. The excess loss of a 50 mm long coupler is about 0.7 dB including
waveguide and fibre coupling losses. A novel method is proposed for tuning the
coupling ratio. By bending the coupler, high precision control of within 1% is
attained without optical polarisation dependence.
151. S. Zhang and N. Kobayashi
"Using
Tertiary Butylamine For Nitrogen Doping During Migration-Enhanced
Epitaxial-Growth Of Znse"
Jpn.
J. Appl. Phys. Part 2 - Lett. 31 (6A), L666-L668 (1992).
ABSTRACT: We
report the first use of tertiary butylamine as a nitrogen source for doping
nitrogen into ZnSe. Tertiary butylamine cracked at various temperatures from
550 to 850-degrees-C was supplied onto ZnSe grown by migration-enhanced
epitaxy. Photoluminescence of the doped ZnSe films indicated that nitrogen
concentration increases with increasing cracking temperature. Secondary ion
mass spectrometry revealed that a uniform nitrogen concentration as high as 8 x
10(18) cm-3 could be achieved. The results of site-selective doping onto Se and
Zn surfaces during growth imply that nitrogen is more efficiently incorporated
into ZnSe when the dopant is supplied at the same time that Se is supplied.
152. S. Zhang and N. Kobayashi
"X-Ray-Diffraction
Study Of Annealed Znse/Gaas Superlattices"
Appl.
Phys. Lett. 60 (20), 2499-2501 (1992).
ABSTRACT: We
investigate the effect of annealing on the structural properties of ZnSe/GaAs
superlattices by the x-ray double-crystal rocking-curve technique. A 6-period
ZnSe/GaAs superlattice with 61-nm thick ZnSe layers and 6-nm thick GaAs layers
is grown by a combination of migration-enhanced epitaxy and solid-phase
epitaxy. X-ray diffraction is measured for the ZnSe/GaAs superlattice samples
annealed at different temperatures for several annealing periods in flowing H-2
gas. From the change in the (004) and (115) rocking-curve profiles with
increasing annealing temperature and annealing period, it was found that about
25% of the parallel strain in the ZnSe layers is relieved by misfit
dislocations after annealing at 520-degrees-C for 20 min. The interface
properties of the annealed ZnSe/GaAs superlattices are also examined by
computer simulation of kinematical diffraction.
153. S. Zhang and N. Kobayashi
"Photoluminescence
From Narrow Znse/Gaas/Znse Quantum-Wells"
J.
Cryst. Growth 117 (1-4), 1074-1074 (1992).
ABSTRACT:
154. S. Zhang and N. Kobayashi
"Photoluminescence
And Structure Properties Of Gaas/Znse Quantum-Wells"
Appl.
Phys. Lett. 60 (7), 883-885 (1992).
ABSTRACT: By
improving the quality of the GaAs well layer on a ZnSe barrier, we were able to
observe the quantum size effect in photoluminescence of ZnSe/GaAs/ZnSe quantum
wells. After solid phase epitaxy of 2-ML GaAs on ZnSe epilayer,
migration-enhanced epitaxy (MEE) of the GaAs well layer was carried out while
the growth temperature was elevated in steps. Photoluminescence from the
obtained quantum wells has been appreciably improved by this method. The photoluminescence
spectra show a systematic shift to higher energies as the well width is
reduced, clearly demonstrating the size effect in the ZnSe-GaAs system. By
comparing the experimental data with calculated emission energies, the
valence-band and conduction-band discontinuities between ZnSe and GaAs in the
<001> direction have been determined to be 1.27 +/- 0.02 and 0.03 +/-
0.02 eV, respectively.
155. S. Zhang, N. Kobayashi,
and Y. Horikoshi
"Growth
And Characterization Of Thin Znse/Gaas/Znse Quantum-Wells"
Surf.
Sci. 267 (1-3), 124-128 (1992).
ABSTRACT:
ZnSe/GaAs/ZnSe single quantum wells (QW's) with a well width as thin as 2 nm
and 15-period ZnSe/GaAs (with a barrier width of 97 nm and a well width of 3
nm) multiple quantum wells have been successfully grown by Migration-Enhanced
Epitaxy (MEE). The structures have been confirmed by transmission electron
microscopy (TEM) and high-resolution scanning electron microscopy (SEM). It has
been also revealed that the quantum well structures are formed coherently on
the GaAs(001) substrate. Furthermore, emissions due to the quantum size effect
in the ZnSe/GaAs system have been achieved in photoluminescence measurements.