1994 (with abstract) |
|
▼ Ordered by first author |
1. T.
Akazaki, J. Nitta, H. Takayanagi, T. Enoki, and K. Arai
"Improving
The Mobility Of An In0.52al0.48as/In0.53ga0.47as Inverted Modulation-Doped
Structure By Inserting A Strained Inas Quantum-Well"
Appl.
Phys. Lett. 65 (10), 1263-1265 (1994).
ABSTRACT: The
mobility of two-dimensional electrons in an In0.52Al0.48As/In0.53Ga0.47As
inverted modulation-doped structure improved by inserting an InAs quantum well
into the InGaAs channel. This letter addresses the main cause of this mobility
improvement. By optimizing the thickness of the InAs quantum well, its distance
from the underlying InAlAs spacer layer, and the InAlAs spacer-layer thickness,
maximum mobilities of 16 500 cm2/V s at 300 K and 155 000 cm2/V s at 10 K are
attained. The improvement in mobility is attributed to a decrease in scattering
caused by ionized impurities, interface-roughness, and trap impurities. This
decrease is a result of the superior confinement of two-dimensional electron
gas in the InAs quantum well.
2. S.
Ando, N. Kobayashi, and H. Ando
"Selective-Area
Metalorganic Chemical-Vapor-Deposition Growth For Hexagonal-Facet Lasers"
J.
Cryst. Growth 145 (1-4), 302-307 (1994).
ABSTRACT: In
order to obtain low threshold hexagonal-facet (HF) lasers by reducing their
size! it is necessary to know the selective growth conditions of a hexagonal
prism on a smaller area. We describe the metalorganic chemical vapor deposition
(MOCVD) growth conditions for GaAs and AlGaAs hexagonal prisms on a SiO2 masked
(111)B substrate. The crystal shape and the facet strongly depend on the size
of the mask windows, on the working pressure during growth, and on the growth
parameters of the substrate temperature and the partial pressure of arsine.
Furthermore, we explain the mechanism of the hexagonal prism growth by using
the change of growth rate between low-index facet planes. By using optimized
growth conditions, a 2 mu m sized I-IF laser structure with flat GaAs/AlGaAs
heterointerface can be grown.
3. H.
M. Appelboom, H. Sato, and M. Naito
"Lanthanum
And Calcium-Doped Yba2cu3oy Films Grown At Low-Temperature And Pressure"
Physica
C 221 (1-2), 125-135 (1994).
ABSTRACT: We
have fabricated lanthanum and calcium doped YBa2Cu3Oy films with co-evaporation
at low oxygen/ozone pressures according to the stoichiometric formulae
YLaxBa2-xCu3Oy and Y1-xCaxBa2Cu3Oy. The lanthanum doped films show a strong
reduction or absence of solid solubility of lanthanum on the barium site
compared to bulk material made at atmospheric oxygen pressure, analogous to what
has been reported previously for Sm1+xBa2-xCu3Oy films [Physica C 214 (1993)
323]. In the calcium doped films we find a solid solubility limit which is
apparently similar to that reported for bulk material synthesized at
atmospheric oxygen pressure. The reduction of solid solubility in the
YLaxBa2-xCu3Oy system is explained by a shift of the low oxygen pressure
decomposition line to higher pressure with lanthanum doping. We also report
here on the successful synthesis of oxygen-deficient superconducting Y1-xCaxBa2Cu3O6
films.
4. E.
Atsumi, M. Takagi, and K. Yokosawa
"Local
Motion Detection By Hierarchical Neural-Network"
Syst.
Comput. Jpn. 25 (11), 24-35 (1994).
ABSTRACT:
Perception of visual motion is thought to consist of two stages: generation of
candidates and their interaction to determine true motion. In this paper, a
three-layered neural network is applied to detect local visual motion. The
network, after learning, could categorize nine types of motion and obtained a
motion detection algorithm that included the two states of perception. The
internal representations for the first stage agree with the functions of
on-center and off-center cells, and those for the second stage agree with the
functions of lateral inhibition. We also tried to detect arbitrary motions by
combining multi-resolution representation of images with the neural network.
5. T.
Bever, Y. Hirayama, and S. Tarucha
"Quantized
Conductance In Ingaas Point Contacts At High-Temperatures"
Jpn.
J. Appl. Phys. Part 2 - Lett. 33 (6A), L800-L803 (1994).
ABSTRACT: We
used focused ion beam insulation writing to fabricate quantum point contacts in
the two-dimensional electron gas of an InGaAs/InAlAs heterostructure. The
conductance as a function of voltage on an adjacent in-plane gate exhibited
steps for temperatures up to 60 K. From the temperature and source-drain
voltage and magnetic field dependence of the conductance steps, we estimated
the one-dimensional subband spacing to be 15 meV.
6. T.
Bever, Y. Hirayama, and S. Tarucha
"Strong
Negative Transconductance In In-Plane-Gate Transistors Written By
Focused-Ion-Beam Implantation"
J.
Appl. Phys. 75 (11), 7573-7575 (1994).
ABSTRACT: A
strong negative transconductance is investigated in in-plane-gate transistors
written by focused-ion-beam implantation in the two-dimensional electron gas in
modulation-doped AlGaAs/GaAs heterostructures. This occurs in a configuration
where two in-plane gates G1 and G2 used to control the current through a
channel lying between them are biased with different voltages V(g1), and V(g2).
When the voltage V(g2)<0 is held constant, the current through the channel
can be reduced to zero by increasing V(g1) beyond a critical value. In an
earlier study this effect was attributed to velocity modulation. It is found,
however, that in this regime V(g1) causes a very small current I(g2) to flow
across gate G2. It is observed that changes in I(d) are correlated to changes
in I(g2) and thus conclude that I(g2) is responsible for the strong negative
transconductance.
7. T.
Bever, Y. Hirayama, and S. Tarucha
"Enhanced
Collimation In Narrow Channels Fabricated By Focused-Ion-Beam
Implantation"
J.
Appl. Phys. 75 (5), 2477-2480 (1994).
ABSTRACT: We
investigate the collimation factor of narrow channels defined by focused-ion-beam
insulation writing in the highly mobile two-dimensional electron gas of an
AlGaAs/GaAs heterostructure. We show that the degree of collimation can be
enhanced by appropriate channel design. Additional boundary roughness caused by
selective implantation of ions along the channel boundary considerably
increases the collimation.
8. G.
Bjork, A. Karlsson, and Y. Yamamoto
"Definition
Of A Laser Threshold"
Phys.
Rev. A 50 (2), 1675-1680 (1994).
ABSTRACT: We
propose that the threshold of a laser is more appropriately described by the
pump power (or current) needed to bring the mean cavity photon number to unity,
rather than the conventional ''definition'' that it is the pump power at which
the optical gain equals the cavity loss. In general the two definitions agree
to within a factor of 2, but in a class of microcavity lasers with high
spontaneous emission coupling efficiency and high absorption loss, the
definitions may differ by several orders of magnitude. We show that in this
regime the laser undergoes a transition from a linear (amplifier) behavior to a
nonlinear (oscillatory) behavior at our proposed threshold pump rate. The
photon recycling resulting from the high spontaneous emission coupling
efficiency and high absorption may in this case result in lasing without
population inversion, and coherent light is generated via ''loss saturation''
instead of gain saturation. This mechanism for lasing without inversion is very
different from lasing without inversion using a radiation trapped state.
9. G.
Bjork, S. Pau, J. Jacobson, and Y. Yamamoto
"Wannier
Exciton Superradiance In A Quantum-Well Microcavity"
Phys.
Rev. B 50 (23), 17336-17348 (1994).
ABSTRACT:
10. S. J.
Chang and K. Takahei
"Studies
Of Gaaser Impact Excited Electroluminescence Devices"
Appl.
Phys. Lett. 65 (4), 433-435 (1994).
ABSTRACT: We
report on the study of impact excitation of Er ions in GaAs. The metalorganic
chemical vapor deposition grown, p+-n structured electroluminescence (EL)
devices were fabricated by growing, at different temperatures, GaAs:Er layers
on top of the n+ GaAs substrates. P+ layers of GaAs were made by Zn diffusion
from the top surfaces. When we forward biased these diodes, the EL spectra were
similar to the respective photoluminescence (PL) spectra of each sample. The
spectra of the samples differed for the various growth temperatures. However,
when we reverse biased these diodes, the EL spectra are the same for all
samples but different from the PL spectra. These results indicate that the Er
center(s) excited by direct impact is different from the Er center(s) excited
through electron-hold recombination and the subsequent energy transfer.
11. A.
Chavezpirson, H. Ando, H. Saito, and H. Kanbe
"Quantum-Wire
Microcavity Laser Made From Gaas Fractional Layer Superlattices"
Appl.
Phys. Lett. 64 (14), 1759-1761 (1994).
ABSTRACT: We
report the first demonstration of lasing action in a quantum wire microcavity
semiconductor laser made from an array of (AlAs)1/4(GaAs)3/4 fractional-layer
superlattice (FLS) quantum wires. The FLS growth method produces uniform,
densely packed, damage-free arrays of nanometer-size quantum wires which are
integrated into an optical microcavity that is the size of the wavelength of
the light. We obtain room temperature optically pumped lasing for wavelengths
from 670 to 690 nm. The lasing output is linearly polarized parallel to the
quantum wires, reflecting the higher optical gain for polarization direction
parallel to the wires. The combination of a semiconductor quantum wire active
material with an optical microcavity offers the possibility of ultimately
compact, highly efficient laser sources.
12. S.
Friberg
"Quantum-Wire
Microcavity Laser Exhibits Unique Modulation Properties"
Laser
Focus World 30 (9), 80-80 (1994).
ABSTRACT:
13. S.
Friberg
"Noninvasive
Readout Technique Preserves Soliton Signal"
Laser
Focus World 30 (1), 15-16 (1994).
ABSTRACT:
14. M.
Fujiki
"Optically-Active
Polysilane Homopolymer - Spectroscopic Evidence Of Double-Screw-Sense Helical
Segmentation And Reconstruction Of A Single-Screw-Sense Helix By The
Cut-And-Paste Technique"
J.
Am. Chem. Soc. 116 (26), 11976-11981 (1994).
ABSTRACT: We
have studied the skeleton conformation of optically active polysilane
homopolymer, poly(methyl((S)-2-methylbutyl)silane) (1), as a model of flexible
chainlike polymers in solution, by means of various optical spectra (UV
absorption, circular dichroism, fluorescence, fluorescence excitation, and
fluorescence anisotropy), NMR spectra (C-13 and Si-29), intrinsic viscosity as
a function of molecular weight of polymer, screw-sense-selective photolysis,
and GPC analysis equipped with a photodiode array UV detector. From a
comparison among its circular dichroism, UV absorption, fluorescence, and
fluorescence excitation spectra, we concluded that both P-screw-sense, tight
helical and M-screw-sense, loose helical segments coexist in the same chain of
1-diastereomeric helical segment-like block structure. The
screw-sense-selective photolysis suggests that segments responsible for P- and
M-screw-senses consist of nine silicon atoms. On the basis of this
conformational model, modified 1* with almost a single P-screw-sense was
reconstructed by the screw-sense-selective ''cut-and-paste'' procedure used for
original 1.
15. M.
Fujiki
"Effect
Of Main-Chain Length In The Exciton Spectra Of Helical-Rod Polysilanes As A
Model Of A 5-Angstrom Wide Quantum-Wire"
Appl.
Phys. Lett. 65 (25), 3251-3253 (1994).
ABSTRACT:
16. M.
Fujiki
"Ideal
Exciton Spectra In Single-Screw And Double-Screw Sense Helical
Polysilanes"
J.
Am. Chem. Soc. 116 (13), 6017-6018 (1994).
ABSTRACT:
17. T.
Fujisawa, T. Bever, Y. Hirayama, and S. Tarucha
"Nanostructure
Fabrication And The Science Using Focused Ion-Beams"
J.
Vac. Sci. Technol. B 12 (6), 3755-3759 (1994).
ABSTRACT:
18. T.
Fujisawa, Y. Hirayama, and S. Tarucha
"Algaas/Ingaas/Gaas
Single-Electron Transistors Fabricated By Ga Focused Ion-Beam
Implantation"
Appl.
Phys. Lett. 64 (17), 2250-2252 (1994).
ABSTRACT:
Single electron transistors are formed in an AlGaAs/InGaAs/GaAs
modulation-doped heterostructure by Ga focused ion beam implantation. The
AlGaAs/InGaAs/GaAs system has a high two-dimensional electron gas density and
facilitates a lateral constriction whose depletion length is much smaller than
that in a conventional AlGaAs/GaAs system. A dot structure confined by a small
depletion spreading of less than 0.15 mum is formed by the ion implantation.
This ion implantation is also employed to form in-plane gates for controlling
the tunneling junctions between the dot and reservoirs, and the number of
electrons in the dot. Coulomb oscillations and a Coulomb staircase have been
clearly observed by controlling three in-plane gates.
19. T.
Fukuda
"Determination
Of Silver Coverage On Si(111) 3x1 (6x1)-Ag Surfaces"
Phys.
Rev. B 50 (3), 1969-1972 (1994).
ABSTRACT: The
number of silver atoms incorporated into a Si(111)3 X 1(6 X 1)-Ag structure is
determined by scanning tunneling microscopy (STM) and Auger electron
spectroscopy (AES). Silver MNN Auger intensities from surfaces with two
different compositions were compared between clean 7 X 7, (square-root 3 X
square-root 3)R 30-degrees-Ag, and 3 X 1(6 X 1)-Ag structures, which were
determined from scanning tunneling microscopy images. From the AES intensity
ratio and known occupancies of each reconstruction, the number of Ag atoms
incorporated into the 3 X 1(6 X 1)-Ag structure was determined to be 0.
36+/-0.16 ML. This value is close to 1/3 ML, suggesting that one of the two
rows observed by STM does not consist of Ag atoms.
20. T.
Fukuda
"Preservation
Of The Phase-Boundary Of Si(111) 7x7 Structure In Air Studied By Force
Microscopy"
Jpn.
J. Appl. Phys. Part 2 - Lett. 33 (6A), L797-L799 (1994).
ABSTRACT:
Si(111) surfaces cleaned under ultrahigh vacuum were studied by force
microscopy in air. 7 x 7 domain boundaries associated with the phase transition
from 1 x 1 to 7 x 7 during cooling were imaged as 1.0 approximately 1.5
angstrom high protrusions. The morphology was quite consistent with results
from in situ techniques. For rapidly quenched surfaces, disordered 1 x 1
triangles were also seen in the middle of terraces. These structures may be
related to the difference in surface atom densities and the difference in
reaction to oxygen.
21. U.
Geigenmuller and M. Ueda
"Nonadiabatic
Analysis Of The Josephson Critical-Current Influenced By Quantum Phase
Fluctuations"
Phys.
Rev. B 50 (13), 9369-9375 (1994).
ABSTRACT: The
influence of the electromagnetic environment on the dc Josephson current is
studied allowing for nonadiabatic motion of the phase difference across a
junction. The critical current is evaluated nonperturbatively within mean-field
theory, fully taking into account the nonlocal kernels in the
Ambegaokar-Eckern-Schon effective action. It turns out that the adiabatic
approximation, which can be justified when the superconducting energy gap
exceeds the charging energy, yields qualitatively correct results even for the
opposite case, although quantitative deviations from the adiabatic
approximation are found to be substantial in some experimentally accessible
regions.
22. U.
Geigenmuller and M. Ueda
"Suppression
Of The Josephson Current By Quantum Phase Fluctuations - Beyond The Adiabatic
Approximation"
Physica
B 194, 1005-1006 (1994).
ABSTRACT: We
study how the Josephson current in a shunted junction is suppressed when the
energy gap DELTA is not large compared to the charging energy E(C). Then the
time dependence of the nonlocal kernels in the effective action describing the
junction becomes important. For low ratios of the Josephson energy to E(C), the
Josephson current deviates by tens of percent from what one obtains in the
adiabatic limit (i.e. DELTA >> E(C)).
23. M.
Georgiou, P. Mandel, and K. Otsuka
"Modulation
Of A 2-Model Laser"
IEEE
J. Quantum Electron. 30 (3), 854-859 (1994).
ABSTRACT: We
analyze a two-mode laser; described by rate equations, whose gain is
periodically modulated. The nature of the response varies significantly with
the modulation amplitude. We study both the small modulation in which the pump
parameter remains always above the lasing threshold for the second mode, and
the deep modulation in which the pump parameter is located during part of
the,cycle between the single-mode and the two-mode thresholds. Apart from the
strong McCumber nonlinear resonance at the relaxation oscillation frequency, we
describe a rich variety of nonlinear properties such as multistability among
periodic and quasi-periodic solutions, and small resonances in the vicinity of
the second (and lower) internal frequency. We also identify domains that
suggest the occurrence of the traditional routes to chaos.
24. O.
Hasegawa, M. Ishizuka, and K. Yokosawa
"Realtime
Parallel And Cooperative Recognition Of Human Face For A Naturalistic Visual
Human Interface"
Syst.
Comput. Jpn. 25 (11), 11-23 (1994).
ABSTRACT: The
concept of a Visual Software Agent (VSA), i.e., an anthropomorphic agent
possessing a realistic human form and communication functions that create an
interface with the user, is proposed. Research is proceeding on its
implementation on a parallel computer. In this paper, we describe a method that
is effective as the visual input function of the anthropomorphic agent. This
method recognizes and extracts only one person (user) directly facing the
camera in a moving image in which several people occasionally enter and leave.
The recognition method can be executed in real time in a typical indoor
environment. The background and the lighting do not have to be restricted and
recognition can be achieved in real time by a parallel computer. In addition,
this technique simulates the initial stage of human visual functions and is
based on the parallel extraction and integration of multiple image features.
The movements of visual attention of cognitive psychology can also be
simulated. An anthropomorphic agent derived from this approach successively
looks at multiple human faces, fixes its gaze only on a specific person, and
synthesizes agent behavior that approximate that of humans. These moving image recognition
and synthesis processes were implemented on a newly designed parallel computer.
25. I.
Hashimoto, T. Mashiko, T. Mizuta, T. Imada, K. Iwase, and H. Okazaki
"Visualization
Of A Moving Quadrupole With Magnetic Measurements Of Peripheral-Nerve Action
Fields"
Electroencephalogr.
Clin. Neurophysiol. 93 (6), 459-467 (1994).
ABSTRACT:
Magnetic compound action fields (CAFs) over the right arm were measured from 63
sensor positions with two 7-channel SQUID gradiometer systems following
electrical stimulation of the median nerve at the wrist. The field mapping of
the CAFs revealed a propagating quadrupolar pattern with the leading
depolarization and trailing repolarization fronts. The average distribution of
the CAFs in the longitudinal direction was 9.0 cm in length for the
depolarization field and 7.3 cm for the repolarization field in good agreement
with a theoretical prediction based on the duration (3 msec) of the CAFs and
the conduction velocity of the nerve (50 m/sec); The distance between the maxima
of the depolarization front and the minima of the repolarization front was 6.3
cm. This spatial separation of the learning and trailing dipole locations
suggests in part mutual cancellation of the fields with opposite polarity at or
near the depolarized segment of nerve fibers.
26. N.
Hatakenaka, S. Kurihara, and T. Ogawa
"Andreev-Reflected
Photons"
Physica
B 194, 1699-1700 (1994).
ABSTRACT: We
investigate theoretically the Andreev-reflected photons in a system with two
vacuum-semiconductor and semiconductor-superconductor interfaces, taking into
account the multiple reflections of a polariton at two interfaces. With the use
of the Andreev reflection of an electron-hole pair in this geometry, we propose
a novel generation scheme of a phase-conjugated photon with respect to the
incident one. This mechanism is quite different from conventional methods using
optical nonlinearities. The additional-boundary-condition problems axe also
reexamined from a viewpoint of an electron-hole picture.
27. N.
Hatakenaka, T. Ogawa, and S. Kurihara
"Squeezing
Of Photons Through Josephson Tunnel-Junctions"
Physica
B 194, 1701-1702 (1994).
ABSTRACT: We
propose a novel scheme for generating squeezed states of photon, which scheme
is based on a nonadiabatic effect of photons on a two-state system. This is
realized in a Josephson tunnel junction weakly coupled with photon fields in an
optical cavity. The supercurrent fluctuation is also shown to be affected by
its surrounding electromagnetic field as well as by the electronic system.
28. H.
Hayakawa, S. Nishida, Y. Wada, and M. Kawato
"A
Computational Model For Shape Estimation By Integration Of Shading And Edge Information"
Neural
Netw. 7 (8), 1193-1209 (1994).
ABSTRACT: In
constructing a computational model for human perception of shape-from-shading,
we must solve two major problems: (1) How do we estimate the shape within a
small number of iterations? and (2) How do we integrate the shading and edge
information for shape estimation? To solve the first problem, we propose a
solution for the shape-from-shading problem by using forward and approximated
inverse optics. Because the surface normal modification required due to the
brightness error is separated from that required due to the smoothness
constraint, we can use a simple and fast algorithm for each modification. To
solve the second problem, we propose a computational model for shape estimation
by integration of shading and edge information. The model is comprised of three
modules for the surface normal, discontinuity, and light direction estimation.
A rather weak interaction among the three modules can undo the
shape-from-shading problem that resembles the chicken-and-egg problem.
29. O.
Hellman
"Impurity-Mediated
One-Dimensional Crystallization Of Thin Amorphous-Ge Films On Si(111)"
J.
Appl. Phys. 76 (6), 3818-3822 (1994).
ABSTRACT: We
have observed peculiar low temperature crystallization dynamics of thin
amorphous Ge films deposited on Si (111):7X7 substrates. The one-dimensional
geometry and low temperature kinetics of this crystallization indicate an
impurity mediated mechanism similar to that suggested by Nygren, McCallum,
Thornton, Williams, and Olson [Mater. Res. Soc. Symp. Proc. 100, 403 (1988)].
Interaction is observed between the buried surface structure and the
crystallizing Ge film, in some cases resulting in Ge which grows epitaxially
not on the bulk Si, but on the 7X7 reconstruction, effectively a
two-dimensional substrate.
30. O.
Hellman
"Buried
Reconstruction Inhibition Of Solid-Phase Epitaxy Of Ge On Si(111)"
J.
Vac. Sci. Technol. A-Vac. Surf. Films 12 (5),
2825-2829 (1994).
ABSTRACT: We
study the epitaxial crystallization of a thin film of amorphous Ge deposited at
room temperature on Si (111). Silicon surface features which are buried beneath
the Ge film are seen to affect the rate of crystallization. In particular,
solid phase growth is observed to be enhanced at surface steps and defects in
the surface reconstruction. We demonstrate that control of Ge crystallization
morphology is possible through manipulation of Si surface structure.
31. H.
Hibino and T. Ogino
"Scanning-Tunneling-Microscopy
Observations Of Ge Solid-Phase Epitaxy On Si(111)"
Appl.
Surf. Sci. 82-3, 374-379 (1994).
ABSTRACT:
Solid-phase epitaxy (SPE) of Ge on a clean, 7 x 7-reconstructed Si(111) surface
is investigated by scanning tunneling microscopy. Although Ge layers of four
monolayers (ML) thick crystallize in the registry of the 7 x 7 reconstruction
preserved at the amorphous Ge/Si interface, the 7 x 7 reconstruction hardly
influences the SPE of 2 ML thick Ge layers. This difference is due to the
reduced movement of atoms at the interface with thicker overlayers.
32. H.
Hibino and T. Ogino
"Trace
Of Interface Reconstruction In Ge Solid-Phase Epitaxy On Si(111)"
Phys.
Rev. B 49 (8), 5765-5768 (1994).
ABSTRACT: We
describe the mechanism of solid-phase epitaxy (SPE) of Ge on a Si(111)-7 X 7
surface using reflection high-energy electron diffraction and scanning
tunneling microscopy. Amorphouslike Ge layers crystallize in the registry of
the 7 X 7 reconstruction preserved at the Ge/Si interface. The preferred basic
unit of epitaxy is a triangular domain corresponding to four half-units of the
7 X 7 reconstruction. Faultedly stacked (twinned) domains cover almost half of
the surface at the initial stage of SPE because Ge grows epitaxially on both
the unfaulted and faulted halves of the 7 X 7 reconstruction. These twinned Ge
layers are transformed into normally stacked Ge layers above 400-degrees-C.
33. H.
Hibino and T. Ogino
"Transient
Step Bunching On A Vicinal Si(111) Surface"
Phys.
Rev. Lett. 72 (5), 657-660 (1994).
ABSTRACT: We
used high-temperature scanning tunneling microscopy to observe, in real time,
the step rearrangement induced by a (7 x 7) reconstructive phase transition on
a vicinal Si(111) surface misoriented toward [112BAR]. A new transient step
bunching is found between a high-temperature phase consisting of single-layer
steps with nonreconstructed terraces and a low-temperature phase of a mixture
of single-and triple-layer steps with (7 x 7) reconstructed terraces. The
transient step bunching indicates that the free energy of the (7 x 7)
reconstructed step edge is larger than that of the nonreconstructed step edge
just below the phase transition temperature.
34. H.
Hibino, N. Shimizu, K. Sumitomo, Y. Shinoda, T. Nishioka, and T. Ogino
"Pb
Preadsorption Facilitates Island Formation During Ga Growth On Si(111)"
J.
Vac. Sci. Technol. A-Vac. Surf. Films 12 (1),
23-28 (1994).
ABSTRACT: On
a clean Si(111)-7X7 surface, Ge grows in the Stranski-Krastanov mode. At
300-450 degrees C, relaxed islands begin to form when. the Ge growth is 6
monolayers (ML) thick. When Ge is grown on a Pb/Si(111)-root 3X root 3 surface,
Pb segregates on the surface and agglomerates into two-dimensional islands. And
the critical thickness for the formation of relaxed island becomes 4 ML. This
change in critical thickness is explained by Pb reducing the surface energy or
by an improved crystallinity of Ge layers (due to a simplified substrate
surface reconstruction), or by both.
35. Y.
Hirota
"Effects
Of Dissolved-Oxygen In A Deionized Water-Treatment On Gaas Surface"
J.
Appl. Phys. 75 (3), 1798-1803 (1994).
ABSTRACT:
This article presents a new passivation method with an As and/or hydrogenated
As layer on a GaAs surface. X-ray photoelectron spectroscopy was employed to
investigate the influences of dissolved oxygen on a GaAs surface during the
de-ionized water treatment. It is shown that reduction of dissolved oxygen in
de-ionized water accelerates the removal of Ga and As oxides from the surface,
and that the de-ionized water treatment in an extremely low concentration of
dissolved oxygen produces arsenic and/or hydrogenated arsenic layer due to the
liberation of Ga atoms near the surface. These phenomena are discussed based on
the chemical reaction between the GaAs surface and dissolved oxygen in
de-ionized water. The arsenic and hydrogenated arsenic layer is available for
preserving the oxide-free and damage-free GaAs surface.
36. Y.
Hirota, T. Ogino, Y. Watanabe, and M. Oshima
"Synchrotron-Radiation
Photoelectron-Spectroscopy Study For Gaas (001) Surface Prepared By
Deoxygenated And Deionized Water-Treatment"
Appl.
Phys. Lett. 65 (16), 2036-2038 (1994).
ABSTRACT: The
thermal effects on an n-type GaAs (001) surface prepared by deoxygenated and
de-ionized water (DODIW) treatment are investigated by synchrotron-radiation
photoelectron spectroscopy (SRPES) in the temperature range from room
temperature (RT) to 500-degrees-C. SRPES confirms there are no oxides. There
is, however, excess elemental arsenic and/or hydrogenated arsenic on the
surface before heating, which evaporates when heated in a high vacuum. SRPES
also shows that the surface Fermi level lies almost 0.9 eV above the maximum of
valence band before heating, and moves toward the midgap during heating. After
cooling to RT, it returns to the near-flat band position (1.0 eV). These
experimental results suggest that DODIW-treated GaAs (001) surface can attain a
low-density surface state. (C) 1994 American Institute of Physics.
37. Y.
Horikoshi, M. R. Fahy, M. Kawashima, K. Furukawa, M. Fujino, and N. Matsumoto
"A
New Si Doping Source For Gaas Growth By Molecular-Beam Epitaxy"
Jpn.
J. Appl. Phys. Part 2 - Lett. 33 (3B), L413-L416 (1994).
ABSTRACT: A
new Si cluster material, tertiary-butyloctasilacubane (tBuSi)8, is used as an
efficient Si doping source for molecular beam epitaxy of GaAs. The vapor
pressure of this material varies according to an activation energy of 1.51 eV.
A Si concentration of 2 x 10(20) /cm3 is obtained at a Si cluster cell
temperature of 210-degrees-C and a GaAs growth rate of 1 mum/h. Although the
grown layers suffer from heavy carbon contamination from the Si cluster, this
problem can be alleviated by increasing the substrate temperature.
38. Y.
Horikoshi and S. Minagawa
"Metalorganic
Vapor-Phase Epitaxy 1994 - Proceedings Of The 7th International-Conference On
Metalorganic Vapor-Phase Epitaxy - Yokohama, Japan, 31-May-1994 3-June-1994 -
Preface"
J.
Cryst. Growth 145 (1-4), R9-R10 (1994).
ABSTRACT:
39. T.
Horiuchi, O. Niwa, and H. Tabei
"Detection
Of Reversible Redox Species By Substitutional Stripping Voltammetry"
Anal.
Chem. 66 (8), 1224-1230 (1994).
ABSTRACT: We
have achieved the highly sensitive electrochemical detection of reversible
redox species by a new type of stripping analysis named substitutional
stripping voltammetry (SSV). This analysis requires an interdigitated array
(IDA) microelectrode in a sample solution Combined with a macroelectrode in a
second cell. The second cell contains an electroactive species which deposits
reversibly on the electrode: The charge generated by the redox cycling reaction
of the sample at the IDA is transmitted to the macroelectrode and accumulated
by the deposition of metal ion species on the macroelectrode. A large signal
can be obtained immediately by stripping the deposited species. A linear
relationship was achieved between the concentration and the stripping peak current
when ruthenium hexaammine was used as the sample and silver ions were used as
the reversibly deposited species. A very low detection limit of 10 pmol/dm(3)
was also obtained because the underpotential deposition of silver ions
accompanies the ruthenium hexaammine redox cycling. This is because the
stripping peak potential is different from that of ordinary deposition which
occurs in the initial stage of the potential scan of the macroelectrode. The
charge accumulation by SSV is superior to the electrical integration of the
redox current of ruthenium hexaammine at the IDA.
40. R. Hull,
J. C. Bean, L. J. Peticolas, B. E. Weir, K. Prabhakaran, and T. Ogino
"Misfit
Dislocation Propagation Kinetics In Ge(X)Si(1-X) Ge(100) Heterostructures"
Appl.
Phys. Lett. 65 (3), 327-329 (1994).
ABSTRACT: We
report measurements of misfit dislocation propagation velocities in GexSi1-x
epilayers grown upon Ge(100) substrates, as opposed to the more usual Si(100)
substrates. This geometry allows us to study structures with high Ge
concentration (x greater-than-or-equal-to 0.8) and to compare with previous
extensive measurements for lower Ge concentration layers (x
less-than-or-equal-to 0.35) grown upon Si(100). It is found that all data are
well described by a misfit dislocation velocity which is linear with excess
stress, and which incorporates a compositionally dependent activation energy
with linear interpolation between bulk values for Si and Ge. The combined data
sets from structures grown on Si(100) and Ge(100) substrates is analyzed in the
framework of the diffusive double kink model for dislocation motion.
41. B.
Huttner and A. K. Ekert
"Information
Gain In Quantum Eavesdropping"
J.
Mod. Opt. 41 (12), 2455-2466 (1994).
ABSTRACT: We
analyse the information obtained by an eavesdropper during the various stages
of a quantum cryptographic protocol associated with key distribution. We
provide both an upper and a lower limit on the amount of information that may
have leaked to the eavesdropper at the end of the key distribution procedure.
These limits are restricted to intercept/resend eaves-dropping strategies. The
upper one is higher than has been estimated so far, and should be taken into
account in order to guarantee the secrecy of the final key, which is subsequently
obtained via the so-called privacy amplification.
42. A.
Imamoglu and Y. Yamamoto
"Quantum
Monte-Carlo Wave-Function Approach To Dissipative Processes In Mesoscopic
Semiconductors"
Phys.
Lett. A 191 (5-6), 425-430 (1994).
ABSTRACT: We
extend the quantum Monte Carlo wave-function approach of quantum optics to
analyze the dissipative electron-phonon interaction in semiconductors. The
non-unitary time-evolution of a stochastic wave-function by an effective
Hamiltonian is combined with continuous ''gedanken measurements'' of phonon
emission events, to simulate the electron dynamics.
43. A.
Imamoglu and Y. Yamamoto
"Turnstile
Device For Heralded Single Photons - Coulomb-Blockade Of Electron And Hole
Tunneling In Quantum-Confined P-I-N Heterojunctions"
Phys.
Rev. Lett. 72 (2), 210-213 (1994).
ABSTRACT: We
show that if a double-barrier mesoscopic p-i-n heterojunction is driven by an
alternating voltage source, then Coulomb blockade and quantum confinement
effects together can suppress the quantum fluctuations usually associated with
electron and hole injection processes in semiconductors. It is therefore
possible to generate heralded single-photon states without the need for a
high-impedance current source. Since the frequency of the alternating voltage source
determines the repetition rate of the single-photon states and the magnitude of
the junction current, the present scheme promises high precision photon-flux
and current standards.
44. F.
Ishiyama and K. Otsuka
"Intensity
Probability-Distribution Of Spiking-Mode Oscillations In Lasers - Power-Law
Universality"
Int.
J. Bifurcation Chaos 4 (1), 225-230 (1994).
ABSTRACT: We
theoretically investigated the probability distributions of the output
intensity of lasers with external perturbations. These perturbations were loss
modulation and incoherent delayed feedback. We found that the intensity
probability distributions usually obey a distinct power-law in spiking-mode
oscillations both in periodic and chaotic regimes.
45. T. Ito,
K. Shiraishi, and T. Ohno
"A
Monte-Carlo Simulation Study For Adatom Migration And Resultant Atomic
Arrangement In Alxga(1-X)As On A Gaas(001) Surface"
Appl.
Surf. Sci. 82-3, 208-213 (1994).
ABSTRACT: The
Monte Carlo method is applied to investigate adatom migration of cations in
Al(x)Ga1-xAs (x = 0, 0.5 and 1.0) and the resultant atomic arrangements on a
reconstructed As-stabilized GaAs(001) surface in the adatom coverage range of
theta less-than-or-equal-to 0.5. Cation adatom migration strongly depends on
the adatom coverage on the surface. Randomly impinging cations occupy lattice
sites on the As dimers at the low coverage of theta less-than-or-equal-to 0.1.
As the coverage increases in the range of 0.1 < theta less-than-or-equal-to
0.3, impinging cations predominantly migrate along the missing dimer rows. At a
higher coverage of theta > 0.3, adatoms tend to favor the lattice sites on
the As dimers including those with non-tetrahedral coordination. In
Al0.5Ga0.5As, lattice sites along the missing dimer are mainly occupied by Al
adatoms, while those on As dimers are favored by Ga adatoms. This is because Al
adatom migration proceeds several times more slowly than Ga adatom migration.
These resultant atomic arrangements are discussed in terms of the coverage
dependence of the migration potential.
46. M. Itoh,
T. Saku, T. Fujisawa, Y. Hirayama, and S. Tarucha
"Transport-Properties
Of Modulation-Doped Structures Grown By Molecular-Beam Epitaxy After Focused
Ion-Beam Implantation"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 33
(1B), 771-774 (1994).
ABSTRACT:
Modulation-doped structures are grown by molecular beam epitaxy after focused
ion beam writing. The growth and implantation chambers are connected in a high
vacuum to minimize the effect of growth interruption. The electron channel is
drastically depleted by the buried Be+ implanted region, but only slightly
depleted by the buried Au+ and AU(2+) implanted regions. This is because Be+
implantation forms a p-type material, while Au+ or Au2+ implaniation leaves
damage only in the n-type material. Be+ implantation is therefore used to
fabricate 0.1 mu m-wide wires with electron mobility of 2.1x10(5) cm(2)/Vs.
47. J. M.
Jacobson, Y. Yamamoto, and A. I. Glu
"A
Quantized-Current Standard Based On Coherent Pi-Pulse Excitation Of A
Quantum-Dot"
Europhys.
Lett. 26 (2), 129-133 (1994).
ABSTRACT: A
quantized-current standard tied to the frequency standard (I = ef) is proposed
based on coherent optical pi-pulse excitation of a quantum dot. Fluctuations in
the current are calculated by averaging the quantum dot density matrix over the
basis states of an incident coherent-state pi-pulse. The effects of a finite
population lifetime (T1) and dipole lifetime (T2) via an appropriate Markoff
approximation are included. We show that a quantized-photocurrent accuracy, (ef
- [I])/ef, of 1 part in 10(4) at a current of I = 1.6 pA (f = 10 MHz) is
possible in a semiconductor quantum dot system operating at 2 K. Such a device
may be useful for the generation of photon number states in quantum optics,
i.e. the realization of a photon current standard.
48. W. Jhe,
M. Ohtsu, H. Hori, and S. R. Friberg
"Atomic
Wave-Guide Using Evanescent Waves Near Optical Fibers"
Jpn.
J. Appl. Phys. Part 2 - Lett. 33 (12A), L1680-L1682 (1994).
ABSTRACT: We
discuss an atomic waveguide that guides atoms in a similar way a quadrupole
mass spectrometer guides charged particles. A two dimensional guiding potential
barrier is produced by repulsive optical dipole forces caused by evanescent
waves from optical fibers. A realization of this new atom optical element is
proposed.
49. T.
Kaburagi and M. Honda
"Determination
Of Sagittal Tongue Shape From The Positions Of Points On The Tongue
Surface"
J.
Acoust. Soc. Am. 96 (3), 1356-1366 (1994).
ABSTRACT:
This paper describes a method for determining the shape of the midsagittal
tongue contour from the positions of points on the tongue surface. The
positions of the points and the tongue shape were measured simultaneously by
using an alternating magnetic field device and an ultrasonic B-mode scanner for
continuous speech utterances. A comparison between the magnetic and the
ultrasonic data revealed that the average measurement difference between the
two types of data was 1.16 mm. The shape of the tongue contour was then
represented by multivariable linear regression of the magnetically determined
positions. The results of the regression analysis showed that the tongue
contour was estimated, from four positions on the tongue, with an average
estimation error of 1.24 mm. This estimation error could be reduced to 0.84 mm
when there was no measurement error between the magnetic and the ultrasonic
data, and it was further reduced to 0.43 mm when the receiver coils of the
magnetic device were positioned optimally on the tongue. It was also shown that
the number of data frames for calculating the regression coefficients could be
reduced, while maintaining the estimation accuracy, by appropriately selecting
data frames. Finally, the tongue shape was estimated successfully for several
phonemes from the magnetically determined positions, thus demonstrating the
usefulness of this method for observing the articulatory configuration of the
tongue.
50. T.
Kaburagi and M. Honda
"An
Ultrasonic Method For Monitoring Tongue Shape And The Position Of A Fixed-Point
On The Tongue Surface"
J.
Acoust. Soc. Am. 95 (4), 2268-2270 (1994).
ABSTRACT: An
ultrasonic method is presented that combines B-mode ultrasonic imaging with
pulsed-transmission ultrasound to image the lateral contour of the tongue and
to detect the position of an ultrasonic sensor placed on the tongue surface in
the same plane. Measurement accuracy was investigated with respect to the
distance between the ultrasonic transducer and the sensor, and with respect to
the tilt and lateral displacement of the sensor. An experiment measured
movements of the tongue during continuous speech.
51. Y.
Kanemitsu, T. Ogawa, K. Shiraishi, and K. Takeda
"Exciton
Confinement On A Spherical-Shell - Visible Photoluminescence From Oxidized Si
And Ge Nanoballs"
J.
Lumines. 60-1, 337-339 (1994).
ABSTRACT: We
report strong visible photoluminescence (PL) at room temperature from oxidized
Si and Ge nanoballs, which are composed of a spherical crystalline core and a
surface oxide layer. To explain the experimental results, a model is proposed
in which excitons are confined to a spherical shell, an interfacial layer
between the crystalline core and the surface oxide layer, and in which the
exciton confinement enhances the PL intensity.
52. M. Kasu
and N. Kobayashi
"Scanning-Tunneling-Microscopy
Study Of 2-Dimensional Nuclei On Gaas Grown By Metalorganic
Chemical-Vapor-Deposition"
J.
Cryst. Growth 145 (1-4), 120-125 (1994).
ABSTRACT:
Two-dimensional (2D) nuclei of GaAs grown on a singular (001) surface by
metalorganic chemical vapor deposition have been observed by using high-vacuum
scanning tunneling microscopy (STM). The 2D nuclei extend in the [110]
direction, which is opposite to that of molecular beam epitaxy growth. The 2D
nucleus-number density is measured from the STM images, and the relation
between the density and the surface diffusion coefficient of Ga species is
obtained from simulation of growth at the surface. The surface diffusion
coefficient is estimated to be 10(-7.0+/-0.9) cm(2)/s at 530 degrees C.
53. M. Kasu
and N. Kobayashi
"Scanning-Tunneling-Microscopy
Study Of Gaas Step Structures On Vicinal Substrate Grown By Metalorganic
Chemical-Vapor-Deposition"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 33
(1B), 712-715 (1994).
ABSTRACT:
Scanning tunneling microscopy (STM) is used to study the step structure of
metalorganic chemical vapor deposition (MOCVD)-grown GaAs on a vicinal
substrate. We passivated the as-grown surfaces with As in a vacuum chamber
connected to the MOCVD system in order to protect it from oxidation during its
transfer to the STM system. The undulation amplitude of the monolayer steps
grown on a surface misoriented in the [110] direction is about twice that of
these grown on a surface misoriented in the [($) over bar 110] direction. On a
substrate at misorientation angles equal to or less than 7.0 degrees, surfaces
show a monolayer step staircase when the growth temperature (T-g) >650
degrees C; step bunching occurs and the vicinal surface decomposed into (001)
terraces and facets on which steps bunch when 575 degrees C less than or equal
to T-g less than or equal to 650 degrees C; and elliptical two-dimensional
islands form between the monolayer steps because of a decrease of Ga diffusion
coefficient when T-g<575 degrees C.
54. T.
Kawabata
"Predictor
Codebook For Speaker-Independent Speech Recognition"
Syst.
Comput. Jpn. 25 (1), 37-46 (1994).
ABSTRACT:
This paper discusses a method to handle the diversified dynamic features of
speech by representing the dynamic features of speech by spectrum predictors
and constructing the codebook containing predictors as the elements. The
effectiveness of the method for speaker-independent speech recognition is
examined. Three kinds of predictor structures, i.e., the forward predictor, the
backward predictor and the interpolator, are examined. The predictor codebook
is constructed by the predictor quantization procedure, which is a small
modification of the LBG algorithm. For the evaluation of the phoneme
recognition level, two kinds statistical evaluation quantities and the phoneme
recognition rate have been considered. It is seen as a result that the
predictor codebook can realize a high phoneme separation capability and the
robustness against the speaker variation. By combining the process actually
into the phrase recognition system, the performance at the continuous speech
recognition level is evaluated. In either case, the codebook with the backward
predictor as the elements exhibited the highest performance.
55. A.
Kawana and H. P. C. Robinson
"A
Programmable Relay Matrix For Parallel Stimulation Of Cultured Neurons On
Planar Electrode Arrays"
J.
Physiol.-London 480P, P2-P2 (1994).
ABSTRACT:
56. Y. Kido,
A. Ikeda, Y. Yamamoto, J. Nakata, H. Yamaguchi, and K. Takahei
"Impact-Parameter
Dependent Stopping Powers For Axially Channeled And Semichanneled Mev He Ions
In Gaas-Er"
Phys.
Rev. B 49 (20), 14387-14396 (1994).
ABSTRACT: We
have investigated the impact-parameter dependence of stopping powers for
axially channeled and semichanneled MeV He ions in Er-sheet-doped GaAs
epitaxial layers grown by molecular-beam epitaxy. Ion channeling analysis using
2.0 MeV He+ coupled with the observation by transmission-electron microscope
has revealed the formation of fine ErAs clusters, whose lattice constant
shrinks and coincides exactly with that of the GaAs host. Thus the Er atoms
take the position corresponding to the tetrahedral interstitial site of the
GaAs lattice. The Er peak energies in the backscattering spectra strongly depend
on the impact-parameter dependent stopping powers, in particular for the
incidence along [110] and the directions slightly tilted from [110] and [100].
We divide the stopping power into two parts-contributions from outer electrons
and from inner electrons of GaAs. The former is calculated from the dielectric
response theory. For the latter, we consider four types of stopping powers
dependent upon impact parameter; (1) Dettmann-Robinson theory, (2) the
binary-encounter model, (3) the binary encounter combined with the
local-density approximation, and (4) the extended-local-electron-density model.
The Er peak energies observed are well reproduced employing model (3).
57. N.
Kobayashi
"In-Situ
Monitoring And Control Of Surface Processes In Metalorganic Vapor-Phase Epitaxy
By Surface Photoabsorption"
J.
Cryst. Growth 145 (1-4), 1-11 (1994).
ABSTRACT:
In-situ surface photo-absorption (SPA) was applied to study the dynamic surface
processes and the static surface structures during metalorganic vapor phase
epitaxy (MOVPE). The static surface structure in MOVPE can be analyzed by the
spectrum in near-ultra-violet and visible regions, which comprises an
anisotropic dielectric response due to the surface dimer bond as well as an
isotropic response probably due to the surface back-bond. Time-resolved spectra
showing dynamic changes of the surface can be measured by the use of optical
multichannel analyzer. The rate of surface decomposition of source molecule and
the rate of desorption of surface species were measured as the change of
reflectivity at a fixed wavelength. The decomposition of source molecules was
characterized quantitatively, and a correlation between the rate of desorption
of group V atoms and the bond strength of a surface back-bond was found. During
heteroepitaxy, the surface exchange of group V atom was monitored in situ, and
the growth was accordingly controlled to suppress this exchange reaction and
obtain a compositionally abrupt interface.
58. N.
Kobayashi and T. Makimoto
"Carbon
Incorporation Mechanism In Atomic Layer Epitaxy Of Gaas And Algaas"
Appl.
Surf. Sci. 82-3, 284-289 (1994).
ABSTRACT: By
an in-situ surface photo-absorption study of the ALE process and carbon atomic
layer doping, an other than the so far proposed carbon incorporation mechanism
via formation of a CH2 bridge bond has been found, i.e. carbon incorporation
via an exchange reaction between dissociated CH3 radicals from TMG and As atoms
of the surface onto which TMG is deposited. We also propose a method for
reducing the carbon incorporation by thermal desorption of the CH3 groups.
59. Y.
Kobayashi and N. Kobayashi
"Effect
Of Strain On Source Gas Decomposition And Group-V Desorption In Metalorganic
Vapor-Phase Epitaxy Studied By Surface Photoabsorption"
J.
Cryst. Growth 145 (1-4), 17-21 (1994).
ABSTRACT: The
decomposition rate of source gas and the desorption rate of group V atom were
measured by surface photo-absorption during metalorganic vapor phase epitaxy
(MOVPE). We found that the decomposition of PH3 on GaAs and InAs surfaces,
which produces a large tensile strain, is slower than that on GaP and InP
surfaces. We also found that P desorption from P-stabilized GaAs and InAs
surfaces, which relieves a large tensile strain, is faster than P desorption
from GaP and InP surfaces, respectively. Strain-enhanced desorption was also
observed for the As-stabilized InP surface. The difficulty of forming the
strained surface bond evidently decreases the rate of decomposition and the
ease of breaking the strained surface bond evidently increases the rate of
desorption.
60. Y.
Kobayashi and N. Kobayashi
"In-Situ
Control Of Strained Heterostructure Growth"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 33
(5A), 2463-2467 (1994).
ABSTRACT:
This paper reports the metalorganic vapor phase epitaxial growth of
pseudomorphic InAs/InP single quantum wells (SQWs) on (001) InP substrates
using in-situ surface photo-absorption (SPA) monitoring, and reports on the
optical characterization of them. By adjusting the arsine flow rate, arsine
exposure time and substrate temperature on the basis of in-situ SPA monitoring,
we are able to grow pseudomorphic InAs/InP SQWs comprising up to 10-monolayer
InAs wells having metallurgically abrupt and atomically flat strained
heterointerfaces. Photoluminescence excitation measurement for an 8-monolayer
InAs well shows energy splitting as large as 0.4 eV between heavy and light
holes subbands, indicating the InAs well layer is coherently strained to a
maximum extent within the critical layer thickness.
61. R. C.
Liu and Y. Yamamoto
"Nyquist
Noise In The Transition From Mesoscopic To Macroscopic Transport"
Phys.
Rev. B 50 (23), 17411-17414 (1994).
ABSTRACT:
62. R. C.
Liu and Y. Yamamoto
"Suppression
Of Quantum Partition Noise In Mesoscopic Electron Branching Circuits"
Phys.
Rev. B 49 (15), 10520-10532 (1994).
ABSTRACT: A
partitioned system of fermions is mathematically equivalent to an assembly of
two-level atoms described by spin operators. A number-phase uncertainty
relation can therefore be derived to describe the noise properties of divided
electrons. We examine both the number (or electron flux) and phase (or electron
wave phase) decorrelation introduced by electron branching in mesoscopic
circuits. Initially Poissonian, this electron number partition noise is
increasingly suppressed by inelastic scattering in the transition from
ballistic to dissipative electron division. Graphical results from our model
show a trend from a coherent spin state in the ballistic regime toward a
number-squeezed spin state in the dissipative regime, even when detrimental
elastic scattering is present.
63. Y.
Maeda, K. Takei, and D. J. Rogers
"Compositional
Microstructures In Co-Cr Films For Magnetic Recording (Vol 134, Pg 315, 1994)"
J.
Magn. Magn. Mater. 137 (1-2), 233-233 (1994).
ABSTRACT:
64. Y.
Maeda, K. Takei, and D. J. Rogers
"Compositional
Microstructures In Co-Cr Films For Magnetic Recording"
J.
Magn. Magn. Mater. 134 (2-3), 315-322 (1994).
ABSTRACT:
Using spin echo Co-59 nuclear magnetic resonance and preferential chemical
etching, we have examined compositional inhomogeneities in Co-Cr based alloy
thin film media for magnetic recording. We found that drastic compositional
separation (CS), which produces highly Co-enriched regions within grains,
occurs in both perpendicular and longitudinal recording media. CS is expected
to promote the change from a continuous to a particulate-type magnetic
microstructure suitable for high density magnetic recording.
65. A.
Matsuda, K. Semba, and T. Watanabe
"Anisotropy
And Impurity Effect In High T-C Superconductors"
Physica
C 235, 1395-1396 (1994).
ABSTRACT: The
impurity effect on both superconducting and normal state properties has been
investigated to clarify the dimensionality of the one-electron state. Our
previous study showed that fully oxidized Ba2Y(Cu1-xZnx)(3) O-7-delta (BYCZO)
shows essentially three-dimensional (3D) behavior. This study extends the work
toward more two-dimensional materials, namely oxygen-deficient BYCZO and
Bi2Sr2Ca(Cu1-xCox)(2)O-8. The electronic system of the former stays in 3D,
while that of the latter behaves essentially in a 2D manner, suggesting that
two-dimensionality is irrelevant to high Tc superconductivity.
66. N.
Mitani and S. Kurihara
"Spin
Gap And High-Temperature Superconductivity"
Phys.
Lett. A 184 (4-5), 374-379 (1994).
ABSTRACT: The
relationship between the spin excitation spectrum and the symmetry of Cooper
pairs in cuprous oxide superconductors is studied. It is found that d-wave
superconductivity in the hole system induces an Ising-type anisotropy in the
effective coupling between Cu spins. The resulting spin gap structure at zero
temperature agrees fairly well with recent neutron experiMentS.
67. M.
Mitsunaga, N. Uesugi, H. Sasaki, and K. Karaki
"Holographic
Motion-Picture By Eu3+-Y2sio5"
Opt.
Lett. 19 (10), 752-754 (1994).
ABSTRACT:
Real-time recording of a moving object was made with persistent spectral hole
burning of a cryogenic Eu3+:Y2SiO5 crystal. In a basic holographic
configuration the ultrastable laser frequency was continuously scanned within
the F-7(0)-5D0 absorption line (typically 200 MHz in 20 s) while the object was
in motion, thus permitting the storage and reconstruction of the moving image.
The success of this motion picture is attributable to (1) the kilohertz-wide
hole width, (2) the quasi-persistent hole lifetime, and (3) the high
hole-burning quantum efficiency of this material.
68. M. S.
Miyauchi
"An
O(Mn) Algorithm For Embedding Graphs Into A 3-Page Book"
IEICE
Trans. Fundam. Electron. Commun. Comput. Sci. E77A
(3), 521-526 (1994).
ABSTRACT:
This paper studies the problem of embedding a graph into a book with nodes on a
line along the spine of the book and edges on the pages in such a way that no
edge crosses another. Atneosen as well as Bernhart and Kainen has shown that
every graph can be embedded into a 3-page book when each edge can be embedded
in more than one page. The time complexity of Bernhart and Kainen's method is
OMEGA(nu(G)), where nu(G) is the crossing number of a graph G. A new O(mn)
algorithm is derived in this paper for embedding a graph G = (V,E), where m =
Absolute value of E and n = Absolute value of V. The number of points at which
edges cross over the spine in embedding a complete graph into a 3-page book is
also investigated.
69. M. S.
Miyauchi
"Topological
Ramsey Theorem For Complete Bipartite Graphs"
J.
Comb. Theory Ser. B 62 (1), 164-179 (1994).
ABSTRACT: An
embedding of a graph into a space is linear if each edge is a straight line
segment. In 1991, Negami showed that for any given knot, link, or spatial graph
there is a sufficiently large complete graph K-n such that every linear
embedding of K-n into a space always contains that knot, link, or spatial
graph. This paper generalizes this result to cover complete bipartite graphs.
The results for complete multipartite graphs and for complete graphs are
obtained as corollaries. (C) 1994 Academic Press, Inc.
70. H.
Murase and S. K. Nayar
"Illumination
Planning For Object Recognition Using Parametric Eigenspaces"
IEEE
Trans. Pattern Anal. Mach. Intell. 16 (12), 1219-1227
(1994).
ABSTRACT:
This correspondence presents a novel approach to the problem of illumination
planning for robust object recognition in structured environments. Given a set
of objects, the goal is to determine the illumination For which the objects are
most distinguishable in appearance from each other. Correlation is used as a
measure of similarity between objects. For each object, a large number of
images is automatically obtained by varying pose and illumination direction.
Images of all objects, together, constitute the planning image set. The
planning set is compressed using the Karhunen-Loeve transform to obtain a
row-dimensional subspace, called the eigenspace. For each illumination
direction, objects are represented as parametrized manifolds in eigenspace. The
minimum distance between the manifolds of two objects represents similarity
between tbe objects in the correlation sense. The optimal source direction is
therefore one that maximizes the shortest distance between object manifolds.
Several experiments have been conducted using real objects. Results produced by
the illumination planner have been used to enhance the performance of an object
recognition system.
71. M. Naito
and H. Sato
"Reflection
High-Energy Electron-Diffraction Study On The Srtio3 Surface-Structure"
Physica
C 229 (1-2), 1-11 (1994).
ABSTRACT:
This paper reports a reflection high-energy electron diffraction investigation
of the surface structures of the (001) and (110) crystal faces of SrTiO3 given
various surface treatments. The as-polished surface has a (1 X 1)
unreconstructed structure on both the (001) and (110) crystal faces. The vacuum
annealed surface has a two-domain (2 X 1) superstructure on the (001) face and
a (4 X 4) structure on the (110) face. The oxygen annealed surface has two
superstructures on the (001) face: a two-domain (square-root 13 X square-root
13-R33.7-degrees) structure and a c(6 X 2) structure, and a (4 X 2) or a (4 X
4) structure on the (110) face. Of these surfaces, the oxygen annealed surface
has the highest quality.
72. K.
Nakada, K. Takeda, and H. Hosoya
"Electronic
Band Structures Of Penta-Heptagonal Carbon Networks"
Theochem-J.
Mol. Struct. 117, 79-86 (1994).
ABSTRACT: The
electronic band structures of planar carbon networks consisting solely of
pentagons and heptagons were calculated. Two delocalized structures analogous
to graphite were proposed as the candidates of the most possible
penta-heptagonal network. The electronic structures of these networks were
found to show rather metallic properties marking quite a contrast to graphite.
73. H.
Nakano and H. Takayanagi
"2nd
Quantization Description Of Andreev Reflection"
Physica
B 194, 1759-1760 (1994).
ABSTRACT: A
second quantization description is given for Andreev reflection. The Andreev
reflection is obtained as an elementary excitation for
superconductor-normal-metal coupled systems. This gives us a powerful tool for
investigating the macroscopic quantum mechanical aspects of Andreev reflection.
74. H.
Nakano and H. Takayanagi
"2nd-Quantization
Description Of Andreev Reflection And The Relation To Quasi-Particle Wave
Approaches"
Phys.
Rev. B 50 (5), 3139-3148 (1994).
ABSTRACT: A
second-quantization description is given for Andreev reflection. We introduce
an effective interaction Hamiltonian for the interface between the
superconductor and the normal metal, which enables us to treat transmission and
reflection consistently. The interaction Hamiltonian couples quasiparticles in
the normal region (N) and Bogoliubov quasiparticles in the superconducting
region (S). It facilitates the description of the elementary excitations of the
SN-coupled system, that are generated by Andreev reflections. Moreover, it naturally
brings us to the description where the effect of macroscopic quantum
fluctuations of the superconducting state on Andreev reflections is considered.
This provides a powerful tool for investigating of the mesoscopic aspects of
Andreev reflection.
75. S.
Nishida, H. Ashida, and T. Sato
"Complete
Interocular Transfer Of Motion Aftereffect With Flickering Test"
Vision
Res. 34 (20), 2707-2716 (1994).
ABSTRACT: It
has been suggested that motion aftereffect with static test patterns (static
MAE) reflects activities at a lower level system that dominantly processes
first-order motion, while MAE with a directionally ambiguous test (flicker MAE)
reveals a higher level system where second-order motion signals as well as
first-order signals are available. To test this hypothesis, we examined
interocular transfer of static and flicker MAE. Flicker MAE should transfer
more efficiently than static MAE if it occurs at a higher level system. In the
first experiment, the adaptation stimulus was a drifting luminance grating
(first-order motion), or a drifting grating defined by flicker or texture
difference (second-order motion). The test stimulus was a luminance grating, either
static or counterphasing. The results indicated that static MAE, which was
induced only by first-order motion, transferred partially, as has been reported
in previous studies, but: the transfer of flicker MAE was nearly perfect with
either first- or second-order adaptation stimuli. The second experiment with
varied adaptation contrast indicated that this complete transfer was not due to
a ceiling effect. These results supported the hypothesis that the underlying
mechanism for flicker MAE is located at a level higher than the mechanism for
static MAE.
76. S.
Nishida, H. Ashida, and T. Sato
"Perfect
Interocular Transfer Of Flicker Motion After-Effect"
Invest.
Ophthalmol. Vis. Sci. 35 (4), 2157-2157 (1994).
ABSTRACT:
77. J.
Nitta, T. Akazaki, and H. Takayanagi
"Anomalous
Magnetic-Field Dependence Of Differential Resistance In A Superconducting
Nb-Inas-Nb Junction"
Physica
B 194, 1757-1758 (1994).
ABSTRACT: The
differential resistance in an InAs-inserted-channel InAlAs/InGaAs
heterostructure coupled superconducting junction is enhanced within the Nb
superconducting gap energy by applying a magnetic field. The enhancement
saturates under a magnetic field of several mT. This behavior suggests that the
pair-potential in the InAs-channel is induced by the superconducting proximity
effect. The magnetic field reduces the penetration of the pair-potential and
the Andreev reflection probability, which causes the enhancement of the
differential resistance.
78. J.
Nitta, T. Akazaki, and H. Takayanagi
"Magnetic-Field
Dependence Of Andreev Reflection In A Clean Nb-Inas-Nb Junction"
Phys.
Rev. B 49 (5), 3659-3662 (1994).
ABSTRACT: The
differential resistance in an InAs-inserted-channel
In0.52Al0.48As/In0.53Ga0.47As heterostructure-coupled superconducting junction
is enhanced within the Nb superconducting gap energy by applying a magnetic
field. However, the enhancement saturates under a magnetic field of several mT.
This behavior suggests the reduction of Andreev-reflection (AR) probabilities
by the magnetic field. The AR probabilities are calculated as a function of the
pair-potential penetration length into the InAs channel. The enhanced AR
probabilities decrease with decreasing pair-potential penetration length. The
magnetic field reduces the penetration of the pair potential in the channel and
therefore reduces the AR probability. This reduction of AR probability causes
an enhancement of dV/dI.
79. O. Niwa,
T. Horiuchi, and H. Tabei
"Electrochemical
Properties Of Carbon-Based Interdigitated Microarray Electrodes Fabricated By
The Pyrolysis Of Electrochemically Prepared Conducting Films"
J.
Electroanal. Chem. 367 (1-2), 265-269 (1994).
ABSTRACT:
80. O. Niwa,
M. Morita, and H. Tabei
"Highly
Selective Electrochemical Detection Of Dopamine Using Interdigitated Array
Electrodes Modified With Nafion Polyester Ionomer Layered Film"
Electroanalysis 6
(3), 237-243 (1994).
ABSTRACT: The
highly selective electrochemical detection of dopamine has been developed using
an interdigitated microarray (IDA) electrode coated with Nafion and polyester
ionomer (Kodak AQ29D) layered films. Because high redox cycling of dopamine can
be maintained in the AQ29D bottom layer, a low detection limit of 50 nmol/dm3
is obtained. Since the upper Nafion layer prevents L-ascorbic acid from
diffusing into the AQ29D layer, the acid concentration in this layer rapidly
decreases when potentiostating one IDA electrode (anode) above and the other
(cathode) below the redox potential of dopamine. This is because L-ascorbic
acid molecules in the AQ29D layer are removed quickly by the electrochemical or
electrocatalytic oxidation at the anode. On the other hand, almost all of the
oxidized dopamine molecules are reduced at the cathode, which maintains a
constant dopamine concentration in the film during measurement. After the
potential step, the influence Of L-ascorbic acid is almost completely
eliminated within a few seconds due to the reduction in acid concentration in
the modified layer. As a result, dopamine can be detected quantitatively at the
cathode in the presence of 100-fold excess Of L-ascorbic acid.
81. O. Niwa
and H. Tabei
"Voltammetric
Measurements Of Reversible And Quasi-Reversible Redox Species Using Carbon-Film
Based Interdigitated Array Microelectrodes"
Anal.
Chem. 66 (2), 285-289 (1994).
ABSTRACT: A
carbon-based interdigitated array (IDA) microelectrode was applied to the
highly sensitive voltammetric detection of reversible and quasi-reversible
redox species in both the anodic and cathodic potential regions. Carbon film
was prepared on a surface-oxidized Si wafer by the pyrolysis of
3,4,9,10-perylenetetracarboxylic dianhydride and was designated as amorphous by
X-ray diffraction and Raman spectroscopy. The Carbon IDA microelectrode was
fabricated by photolithography and dry etching. The IDA electrode had 50
microband pairs. The bandwidth of the IDAs was 3 mu m, and the gap between two
microbands was 2 lambda m. In the measurement of ferrocene derivatives, the iR
drop was negligible when the ferrocene concentration was less than 0.1 mM at a
moderate scan rate due to the low resistivity of carbon film. The cathodic
potential window without redox species extended further in the negative
direction than that of platinum and gold IDAs. The collector current of
ruthenium hexaammine in a generation collection measurement using an IDA agreed
well with the theoretical value even if the sample concentration was in the
tens of nanomoles per liter range due to the flat baseline current at the
collector in the cathodic region and high collection efficiency. The
generation-collection voltammogram of dopamine was greatly improved after
pretreating only the generator electrode. A low detection limit of 10 nM and a
wide linear range from 10 nM to 1 mM were obtained at the collector electrode
because the collector response of dopamine was improved by the generator
pretreatment without increasing the background current at the collector
electrode.
82. T. Ohno
and K. Shiraishi
"Novel
Core Effects In Cs/Gaas(110) Overlayers - Adsorption-Induced Buckling
Enhancement"
Solid
State Commun. 92 (5), 397-400 (1994).
ABSTRACT: The
structural and electronic properties of Cs/GaAs(110) overlayers are
investigated using an ab initio pseudopotential method, in which we include a
''double valence pseudopotential'' (DVPP) to treat Cs 5p core electrons
explicitly. The Cs adsorption enhances the buckling of GaAs(110) surface due to
the Cs 5p, core repulsion, contrary to usual expectations. The buckling
enhancement has a significant effect on the formation of Cs overlayer
structures. The origin of the semiconductor-to-metal transition is also
discussed.
83. M.
Okuya, T. Kimura, R. Kobayashi, J. Shimoyama, K. Kitazawa, K. Yamafuji, K.
Kishio, K. Kinoshita, and T. Yamada
"Single-Crystal
Growth And Anisotropic Electrical-Properties Of (La1-Xcax)2cacu2o6"
J.
Supercond. 7 (2), 313-318 (1994).
ABSTRACT:
Large single crystals of (La1-xCax)2CaCu2O6 were synthesized by the travelling
solvent floating zone (TSFZ) technique. The dimension of the grown boules was
typically 4 mm phi x 30 mm long with the c-axis perpendicular to the growth
direction. After oxygen loading at 1080-degrees-C in 400 atm Of O2, they became
superconductive with a sharp transition at around 50 K. The resistivity was
metallic both along the c-axis and within the ab-plane, with an anisotropy
ratio of gamma2 = (rho(c)/rho(ab)) approximately 50 which is almost independent
of temperature. Details of the crystal growth, heat treatment procedures, and
the results of electrical and magnetic property measurements are presented.
84. K.
Otsuka
"Gain
Circulation And Transverse Effects In Antiphase Laser Dynamics"
Chaos
Solitons Fractals 4 (8-9), 1547-1558 (1994).
ABSTRACT: The
underlying physical processes inherent in self-organized antiphase dynamics in
multi-longitudinal-mode lasers are explored in terms of gain circulation, a new
physical quantity. Transverse effects on antiphase dynamics in
multi-longitudinal-mode lasers are investigated, and three-dimensional
self-organization is shown to result from the cross-saturation dynamics in the
longitudinal and transverse directions.
85. K.
Otsuka
"Ultrahigh
Sensitivity Laser-Doppler Velocimetry With A Microchip Solid-State Laser"
Appl.
Optics 33 (6), 1111-1114 (1994).
ABSTRACT:
Highly sensitive laser Doppler velocimetry featuring the simultaneous
measurement of light-scattering objects moving at different velocities and
vibration sensing based on Doppler-shifted light-injection-induced intensity
modulation in an externally pumped microchip solid-state laser is demonstrated.
86. K.
Otsuka and Y. Aizawa
"Gain
Circulation In Multimode Lasers"
Phys.
Rev. Lett. 72 (17), 2701-2704 (1994).
ABSTRACT:
Self-organized collective behavior in globally coupled multimode lasers is
investigated by introducing a new physical quantity, gain circulation, that
characterizes the gain transfer among lasing modes. Numerical simulations
indicate that the self-organization is established such that the gain
circulations in all the closed interaction paths involving arbitrary multiple
lasing modes become negligibly small as compared with direct mode-to-mode gain
circulations. This implies that the nonreciprocal local (i.e., mode-to-mode)
gain transfers are self-organized so as to ensure reciprocal average gain flow
among modes approximately and that temporal evolutions of individual mode
intensities are determined accordingly.
87. K.
Otsuka and J. L. Chern
"Variation
Of Lyapunov Exponents On A Strange Attractor For Spiking Laser
Oscillation"
Int.
J. Bifurcation Chaos 4 (4), 1053-1060 (1994).
ABSTRACT: We
analyze temporal variations in local Lyapunov exponents for chaotic spiking
lasers in terms of standard deviation and Allan variance as a function of
integral time tau. We show that standard deviations for local Lyapunov
exponents become saturated in short tau regimes. The calculated Allan variance
and power spectrum analysis suggest that the transition between stationary and
nonstationary chaos takes place around the relaxation oscillation period of
lasers, and that local Lyapunov exponents become nonstationary in time in the
short tau regime.
88. K.
Otsuka, D. Pieroux, and P. Mandel
"Modulation
Dynamics And Spatiotemporal Pattern Generation In A Microchip Multimode
Laser"
Opt.
Commun. 108 (4-6), 265-272 (1994).
ABSTRACT:
2N-1 different periodic oscillations are obtained experimentally in a microchip
N-mode laser by different combinations of modulations at multiple relaxation
oscillation frequencies that appear on the basis of antiphase dynamics among
lasing modes. Application of mode-dependent periodic oscillations to generation
of dynamic spatial patterns is demonstrated using a shear plate interferometer.
89. D.
Pieroux, T. Erneux, and K. Otsuka
"Minimal
Model Of A Class-B Laser With Delayed Feedback - Cascading Branching Of
Periodic-Solutions And Period-Doubling Bifurcation"
Phys.
Rev. A 50 (2), 1822-1829 (1994).
ABSTRACT: A
minimal model for a laser with delayed feedback is analyzed. The model is
motivated by two independent studies of a laser controlled by a fully optical
feedback [Otsuka and Chem, Opt. Lett. 16, 1759 (1991)] and a laser with an
optoelectronic feedback [Loiko and Samson, Opt. Commun. 93, 66 (1992)]. By
reformulating the original laser equations in terms of dimensionless
quantities, we obtain a simpler problem which is valid for both lasers. We then
investigate the limit of small-amplitude feedback and small damping and
determine a bifurcation equation for all periodic solutions. We analyze this
condition in terms of increasing values of the delay time and show that each
branch of solutions emerges from the basic state and becomes isolated as the
delay time is progressively increased. The overlap of bifurcating and isolated
branches of solutions explains the coexistence of nearly harmonic and pulsating
solutions. Pulsating solutions may change stability through period-doubling
bifurcation. We determine a simple approximation for this bifurcation point and
study its validity numerically.
90. D.
Pieroux, P. Mandel, and K. Otsuka
"Modulation
Dynamics In A Multimode Laser With Feedback"
Opt.
Commun. 108 (4-6), 273-277 (1994).
ABSTRACT: The
response of an N-mode solid-state laser when the output field is reinjected in
the cavity after N frequency shifts is analyzed. The results obtained with up
to four modes are described and it is tried to infer general rules. The
emphasis is on comparing the dynamics of the partial and the total mode
intensities.
91. F. E.
Pollick, S. Nishida, Y. Koike, and M. Kawato
"Perceived
Motion In Structure-From-Motion - Pointing Responses To The Axis Of
Rotation"
Percept.
Psychophys. 56 (1), 91-109 (1994).
ABSTRACT: We
investigated the ability to match finger orientation to the direction of the
axis of rotation in structure-from-motion displays. Preliminary experiments
verified that subjects could accurately use the index finger to report direction.
The remainder of the experiments studied the perception Of the axis of rotation
from full rotations of a group of discrete points, the profiles of a rotating
ellipsoid, and two views of a group of discrete points. Subjects' responses
were analyzed by decomposing the pointing responses into their slant and tilt
components. Overall, the results indicated that subjects were sensitive to both
slant and tilt. However, when the axis of rotation was near the viewing
direction, subjects had difficulty reporting tilt with profiles and two views
and showed a large bias in their slant judgments with two views and full
rotations. These results are not entirely consistent with theoretical
predictions. The results, particularly for two views, suggest that additional constraints
are used by humans in the recovery of structure from motion.
92. K.
Prabhakaran, T. Nishioka, Y. Kobayashi, and T. Ogino
"In-Situ
Oxidation Of Ultrathin Layers Of Ge On Si(001) - Evidence For Bonding Partner
Exchange"
Appl.
Surf. Sci. 75, 341-347 (1994).
ABSTRACT:
Ultra-thin layers of Ge grown on Si(001) surface are oxidized in situ and
investigated using XPS, AES, MEIS, AFM and TEM. The samples used are Ge layer
formed by deposition at room temperature (RT) and SiGe mixed layer formed by
deposition at 550 degrees C. Oxidation of the RT-grown layer forms GeO on the
surface and on annealing the surface to 360 degrees C, oxygen changes the
bonding partner and forms SiO2, thereby reducing GeO to elemental Ge. In the
SiGe mixed layer, after oxidation, SiO2 and a small amount of GeO are formed.
On annealing, a similar reaction takes place on this surface also, forming SiO2
as the final product on the surface. Air oxidation of the RT-deposited sample
forms Ge suboxides and GeO2 on the surface. GeO is reduced selectively by
annealing at 360 degrees C in vacuum. On the other hand, by rinsing the sample
in warm water, GeO2 is removed selectively.
93. K.
Prabhakaran, T. Nishioka, K. Sumitomo, Y. Kobayashi, and T. Ogino
"Oxidation
Of Ultrathin Sige Layer On Si(001) - Evidence For Inward Movement Of Ge"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 33
(4A), 1837-1838 (1994).
ABSTRACT: An
ultrathin SiGe layer prepared by growing Ge epitaxially on Si(001) was oxidized
and investigated using X-ray photoelectron spectroscopy (XPS) and medium energy
ion scattering (MEIS). Growth at a substrate temperature 550-degrees-C leads to
the formation of a mixed SiCe layer on Si(001). Oxidation of this sample at
250-degrees-C forms predominantly SiO2 and a small amount of GeO. MEIS shows
evidence for the diffusion of Ge inwards by 2-3 angstrom and of Si towards the
surface resulting in the pile up of Ge at the SiO2/SiGe interface. On annealing
the oxidized surface at 360-degrees-C, oxygen leaves the Ge sites and form SiO2
thereby reducing GeO to elemental Ge. The concentration of oxygen remains the
same through out this reaction.
94. K.
Prabhakaran, T. Ogino, T. Scimeca, and M. Oshima
"Interaction
Of Al With Oxidized Ge/Si(001) - A Synchrotron-Radiation
Photoelectron-Spectroscopy Study"
J.
Vac. Sci. Technol. A-Vac. Surf. Films 12 (2),
509-572 (1994).
ABSTRACT:
Interaction of aluminum with an oxidized sample of ultrathin layer Ge (7
angstrom) deposited on Si(001) at room temperature [Ge (7 angstrom)/Si(001) RT]
is studied employing synchrotron radiation photoelectron spectroscopy. Ge (7
angstrom)/Si(001) RT, on exposure to air, forms Ge suboxides, GeO2 and Si
suboxides on the surface. GeO2 is selectively removed completely by rinsing the
sample in warm water, and during this process a small amount of Si oxides is
also formed. Upon depositing Al on this surface, it reacts with oxides of Si
and Ge and forms an overlayer of Al2O3 on the surface, thereby reducing the
oxides to elemental Si and Ge. Further, the reaction is activated by an
increase in surface temperature. In the early stages of the reaction, reduction
of suboxides take place in preference to Si02.
95. K.
Prabhakaran, T. Ogino, T. Scimeca, Y. Watanabe, and M. Oshima
"Bonding
Partner Change Reaction In Oxidation Of Ge On Si(001) - Observation Of 2-Step
Formation Of Sio2"
Appl.
Phys. Lett. 64 (14), 1839-1841 (1994).
ABSTRACT:
Oxidation of 5 angstrom Ge deposited at room temperature on Si(001) and the
dependence of temperature on the oxidation behavior are investigated by
employing synchrotron radiation photoelectron spectroscopy. The sample on
exposure to air forms a mixture of Ge oxides and a small amount of Si oxides.
Upon annealing, oxygen changes its bonding partner from Ge to Si forming SiO2
as the predominant final product. Two distinct steps have been observed in such
a reaction. First step is the cleavage of all the Ge-O bonds and formation of
Si-O bonds to form mainly Si suboxide. The second step is the rearrangement of
Si-O bonds to form SiO2. The former one takes place in the temperature range
200-300-degrees-C whereas the latter one in the range 300-600-degrees-C.
96. K.
Prabhakarana, T. Ogino, R. Hull, J. C. Bean, and L. J. Peticolas
"An
Efficient Method For Cleaning Ge(100) Surface"
Surf.
Sci. 316 (1-2), L1031-L1033 (1994).
ABSTRACT: We
report an efficient method for cleaning Ge substrates similar to the Ishizaka
and Shiraki method for cleaning of Si. The Ge wafers are cleaned in running
deionized water and etched with HF. A thin oxide layer was prepared by dipping
in a mixture of H2O2 and H2O for a few seconds and the oxide layer was removed
by dipping in HF. This procedure was repeated several times to ensure the
removal of several atomic layers of Ge. Finally the thin oxide layer prepared
as described above was thermally decomposed in ultrahigh vacuum by annealing in
the temperature range 300-500-degrees-C. The resulting surface gave rise to
sharp emission peaks due to surface states in UPS illustrating a clean surface.
Impurities such as carbon and oxygen were below detection level in XPS and AES.
Cross sectional TEM studies showed no defects associated with the cleaning
procedure. Ge buffer layer growth and subsequent SiGe growth showed good
morphology and no substrate/buffer defects.
97. H. P. C.
Robinson and A. Kawana
"A
Static Induction Transistor Camera For Fast Fluorescence Imaging"
J.
Physiol.-London 480P, P3-P3 (1994).
ABSTRACT:
98. D. J.
Rogers, Y. Maeda, and K. Takei
"The
Dependence Of Compositional Separation An Film Thickness For Co-Cr And Co-Cr-Ta
Magnetic Recording Media"
IEEE
Trans. Magn. 30 (6), 3972-3974 (1994).
ABSTRACT: The
dependence of the compositional distribution on film thickness was investigated
for Co78Cr22 and Co86Cr12Ta2 films. Spin-echo NMR and preferential chemical
etching revealed that the extent of compositional separation was greatest in
thinner films and decreased during film growth for both Co Cr and Co-Cr-Ta.
Thinner films exhibited enhanced Ms and a higher density of smaller Co-enriched
regions. Ta addition was observed to change the compositional distribution,
promoting a finer pattern of Co enriched regions.
99. D. J.
Rogers, Y. Maeda, K. Takei, J. N. Chapman, J. P. C. Bernards, and C. P. G.
Schrauwen
"Investigations
Of Compositional Separation In Co-Cr Thin-Film Recording Media"
J.
Magn. Magn. Mater. 130 (1-3), 433-441 (1994).
ABSTRACT: We
investigated the effect of a Ge underlayer and substrate temperature during
film deposition (T(s)) on the compositional distribution in Co79Cr21 films
using spin echo nuclear magnetic resonance and preferential chemical etching.
For films deposited at elevated T(s) we observed drastic compositional
separation (CS) leading to a Co enriched phase with approximately 5 at% Cr on
both Ge and polyester. Chemical etching revealed chrysanthemum pattern (CP)
type microstructures. For lower T(s) films we observed less marked CS with a
distinct etched microstructure in the film deposited on Ge and no clear etched
microstructure in the film deposited on polyester. Results from NMR and
chemical etching studies agreed very well with those from X-ray microanalysis.
100. D. J. Rogers, Y. Maeda, K.
Takei, Y. Shen, and D. E. Laughlin
"Investigtions
Of Compositional Separation Of Co-Cr-Ta Cr Thin-Film Recording Media"
J.
Magn. Magn. Mater. 135 (1), 82-88 (1994).
ABSTRACT: The
compositional distribution in Co-Cr-Ta thin films is investigated as a function
of Cr underlayer texture and substrate temperature (T(s)) using spin-echo
nuclear magnetic resonance and preferential chemical etching. Both the extent
and pattern of compositional separation (CS) show no variation with Cr
underlayer texture. Elevated T(s) is observed to promote both CS and grain
boundary Cr enrichment. The magnetic anisotropy fields of Co-enriched
components in the films are observed to increase with T(s), explaining the
T(s), dependence of H(c). Ta addition is observed to control the distribution
of Co and Cr, leading to a unique compositional microstructure which may
enhance the magnetic and recording properties.
101. T. Saku, Y. Horikoshi, and
S. Tarucha
"High-Mobility
Inverted Modulation-Doped Gaas/Algaas Heterostructures"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 33
(9A), 4837-4842 (1994).
ABSTRACT:
High-quality inverted GaAs/AlGaAs modulation-doped heterostructures have been
grown by MBE. An AlAs/GaAs superlattice buffer layer is grown below the AlGaAs
spacer layer to improve the morphology at the inverted heterointerface. An
atomic layer doping and a thick spacer layer are adopted to alleviate the
scattering by ionized donors. The observed electron mobility at 1.5 K is 4.3 x
10(6) cm(2)/Vs at a 2D electron density of 2.8x10(11)/cm(2). Two 2D electron
channels; one formed at the inverted interface and the other at the normal
interface are found to be operative in the observed characteristic. The
electron mobility in the inverted channel is estimated to be as high as 4.9 x
10(6) cm(2)/Vs at an electron density of 2.2 x 10(11)/cm(2), while, in the
normal channel, it is 2.1 x 10(6) cm(2)/Vs at a density of 6 x 10(10)/cm(2).
102. E. T. Sano and Y.
Horikoshi
"Selenium
Doping In Gaas Grown By Molecular-Beam Epitaxy"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 33
(10), 5636-5639 (1994).
ABSTRACT:
Using elementary Se as n-type dopant, Se-doped GaAs films were grown by
molecular beam epitaxy. Characteristics of the films can be classified according
to the amount of Se doped into areas where carrier concentration increases
linearly [area I] (Se concentration less than or equal to 4 x 10(18) cm(-3)),
saturates [area II] (4 x 10(18)-1 x 10(20) cm(-3)) and decreases [area III]
(greater than or equal to 1 x 10(20) cm(-3)). In each area, we found a close
correlation between electrical activity and photoluminescence spectra. The
activation ratio of Se donors was found to be high in the samples classified in
area I. These samples showed an efficient photoluminescence, although the
observed spectra included deep level emissions at 890 nm and 1050 nm in
addition to the band-edge excitonic emission. For the samples in areas II and
III, however, photoluminescence efficiency dropped considerably and only a
broad band emission (1300-1500 nm) appeared. This broad band emission is
probably caused by complexes that include Ga vacancies and Se atoms because
distinct electron concentration saturation takes place in this region.
103. S. Sasaki, A. Matsuda, and
C. W. Chu
"Fermi-Liquid
Behavior And Bcs S-Wave Pairing Of K3c60 Observed By C-13-Nmr"
J.
Phys. Soc. Jpn. 63 (5), 1670-1673 (1994).
ABSTRACT:
This Letter reports on NMR studies of C-13 in K3 C60 above and below T(c) with
an applied field of 2.93 T. It is found that non-single-exponential recovery
data can be fitted by two components and normalized to an identical shape. With
T1 defined in this way, Fermi-liquid behavior is identified above T(c), and a
broadened Hebel-Slichter peak observed below T(c) is well explained by the
Eliashberg theory with 2DELTA(0)/k(B)T(c)=4.31. The possibility of strong
electron correlation and the origin of the multi-exponential recovery are
discussed.
104. M. Sato
"Growth
Of Gaasn By Low-Pressure Metalorganic Chemical-Vapor-Deposition Using
Plasma-Cracked N-2"
J.
Cryst. Growth 145 (1-4), 99-103 (1994).
ABSTRACT:
GaAsN epitaxial layers were grown on GaAs substrates by plasma-assisted
low-pressure metalorganic chemical vapor deposition (MOCVD). Pure N-2 gas, which
is neither corrosive nor toxic, was chosen as the safest nitrogen precursor.
More nitrogen atoms were incorporated from plasma-cracked N-2 than from
plasma-cracked NH3 indicating that N-2 is better precursor for GaAsN growth.
Photoluminescence from GaAsN was red-shifted with increasing nitrogen
concentration. No significant difference was observed in the photoluminescence
results between GaAsN layers grown using the two precursors.
105. T. Sato and S. Nishida
"Does
An Envelope-Detecting Mechanism Mediate Stereopsis For Band-Limited
Stimuli"
Invest.
Ophthalmol. Vis. Sci. 35 (4), 1916-1916 (1994).
ABSTRACT:
106. K. Seki, A. Yuyama, S.
Narioka, H. Ishii, S. Hasegawa, H. Isaka, M. Fujino, M. Fujiki, and N.
Matsumoto
"Uv
Photoelectron-Spectroscopy Of Polysilanes And Polygermanes"
in
Polymeric Materials For Microelectronic Applications, Acs Symposium
Series Vol. 579 (Amer Chemical Soc, Washington, 1994), pp. 398-407.
ABSTRACT: UV
photoelectron spectra were measured for ten polymers with main chains composed
of Si and Ge atoms. The spectra of poly(dialkylsilane)s were described well as
the overlap of the spectra of constituent parts, while polysilanes with aryl
side groups showed the effect of sigma-pi mixing. The spectra of polygermanes
and Si-Ge block copolymers are fairly similar to those of corresponding
polysilanes, while Si-Ge random copolymers show indications of the effect of
the presence of many Si-Ge bonds.
107. K. Semba and A. Matsuda
"Effect
Of Impurity On Anisotropy Of High-Tc Superconductivity In
Yba2(Cu1-Xznx)3o7-Delta Single-Crystals"
Physica
B 194, 1955-1956 (1994).
ABSTRACT: The
effect of Zn doping on anisotropy of high-T(C) superconductivity is studied in
single-crystal YBa2(Cu1-xZnx)3O7-delta (YBCZO) within the range 0<x<0.03.
The resistive transition curves under a magnetic field for these
impurity-containing systems axe successfully described for the first time by
the renormalized fluctuation theory including psi4 term. The derived coherence
length ratio xi(ab)/xi(c), which indicates anisotropy in superconductivity,
decreases as the impurity concentration increases. However, both rho(c) and the
normal state anisotropy rho(c)/rho(ab) increase. This situation is not
consistent with the Lawrence-Doniach (LD) model. The anisotropic 3-D metal
model seems to be appropriate for the YBCZO system. This result excludes
certain types of high-T(c) theories which assume strict two dimensionality of
the electronic system.
108. K. Semba, A. Matsuda, and
T. Ishii
"Normal
And Superconductive Properties Of Zn-Substituted Single-Crystal
Yba2(Cu1-Xznx)3o7-Delta"
Phys.
Rev. B 49 (14), 10043-10046 (1994).
ABSTRACT:
Zn-impurity-induced anisotropy reduction of superconductivity is obtained from
a resistive transition analysis of single-crystal YBa2(Cu1-xZnx)3O7-delta. The
out-of-plane resistivity (rho(c)) increases with Zn doping, while the carrier
concentration remains almost unchanged. The results are not consistent with the
simple Lawrence-Doniach model. Instead, an anisotropic three-dimensional metal
model seems to be promising. A Zeeman-contribution-subtracted magnetoresistance
analysis indicates that a Zn impurity does not cause any magnetic pair
breaking.
109. H. Shibata, K. Kinoshita,
and T. Yamada
"Crystal-Structure
And Growth Of (Ba1-Xsrx)(2)Cu1.1o2.2+Delta(Co3)(0.9) Single-Crystals"
Physica
C 235, 519-520 (1994).
ABSTRACT:
Single crystals of copper-oxycarbonate (Ba1-xSrx)(2)Cu1.1O2.2+delta(CO3)(0.9)
are obtained by solid state recrystallization and their structures are analyzed
by single crystal X-ray diffraction. The size of the crystals are up to 2x2x2
mm(3), and become superconducting at 32K(onset) and 26K(endpoint). Single
crystal X-ray diffraction shows that the crystals have a tetragonal unit cell
with lattice parameters a = 5.570(2)Angstrom and c = 7.868(2)Angstrom, which
are almost equal to those of ceramic samples.
110. H. Shibata, K. Kinoshita,
and T. Yamada
"Single-Crystal
Growth Of (Ba1-Xsrx)2cu1.1o2.2+Delta(Co3)0.9 By Solid-State
Recrystallization"
Physica
C 232 (1-2), 181-183 (1994).
ABSTRACT:
Single crystals of copper-oxycarbonate (Ba1-xSrx)2Cu1.1O2.2+delta(CO3)0.9 are
obtained using abnormal grain growth. Although there are some voids in the
crystals, cubic crystals up to 2x2x2 mm3 are obtained. Electrical resistivity
measurements show that the transition temperature is between 32 K(onset) and 26
K (endpoint), and magnetic susceptibility measurements show about a 25%
shielding volume fraction, which is comparable to the ceramic samples.
111. H. Shibata, A. Matsuda, K.
Kinoshita, T. Watanabe, and T. Yamada
"Origin
Of The Semiconducting-To-Superconducting Transition Of La2-Xca1+Xcu2o6+/-Delta
Under High-Oxygen-Pressure Annealing"
Phys.
Rev. B 49 (17), 12315-12317 (1994).
ABSTRACT: The
Madelung energy of La2-xCa1+xCu2O6+/-delta system, whose properties change from
semiconductor to superconductor under high-oxygen-pressure annealing, is
calculated. We find the, increase in DELTAV(A), the difference in Madelung site
potential between the apex and the CuO2 planes' oxygen, promotes the
superconducting transition in this system. Slight intercalation of oxygen
between two CuO2 planes is found to be of primary importance in determining
DELTAV(A).
112. K. Shiraishi, T. Ito, and
T. Ohno
"Coverage
Dependence Of Migration Potential Of Cation Adatoms On Gaas(001)-(2x4)
Surface"
Solid-State
Electron. 37 (4-6), 601-604 (1994).
ABSTRACT: We
theoretically investigate the migration potential of cation adatoms on the
reconstructed As-rich GaAs (001)-(2 x 4) surface by ab initio calculation. By
increasing the number of cation adatoms, we also study how migration potential
depends on coverage. The calculated results for Ga adatoms suggest that the
long-bridge sites are energetically the most favorable at the iniital stage of
crystal growth. However, as the Ga coverage increases, the missing dimer row
sites become the most favorable. Migration potentials strongly depend on the
adatom coverage. Similar results were obtained for Al adatom migration.
Furthermore, based on these migration potentials, we demonstrate the dynamical
behavior of cation adatoms on GaAs(001) surface by performing Monte-Carlo
simulations at finite temperatures.
113. T. Sogawa, S. Ando, and H.
Kanbe
"Growth
Of Gaas/Alas Trench-Buried Multiple-Quantum Wires By Metalorganic
Chemical-Vapor-Deposition On V-Grooved Substrates"
Appl.
Phys. Lett. 64 (24), 3299-3301 (1994).
ABSTRACT: We
report the fabrication of GaAs/AlAs multiple trench-buried quantum wires (TBWs)
by metalorganic chemical vapor deposition on V-grooved substrates. The shape of
AlAs layers grown on the V-grooves can be changed significantly from a V-shape
to U-shape by varying growth temperatures and group-V/III ratios. 30-nm-wide and
100-nm-deep AlAs trenches with nearly vertical sidewalls are formed at the
growth temperature of 650-degrees-C with the group-V/III ratio of 165, while
V-shaped AlAs grooves are formed at 700-degrees-C with the V/III ratio of 110.
Vertically stacked double TBWs are formed using the 30-nm-wide trenches. The
low-temperature (15 K) photoluminescence spectrum for the double TBWs shows two
distinct emission peaks corresponding to the 6.5- and 8.0-nm-thick wires.
114. T. Sogawa, S. Ando, and H.
Kanbe
"Gaas/Alas
Trench-Buried Quantum Wires With Nearly Rectangular Cross-Sections Grown By
Metalorganic Chemical-Vapor-Deposition On V-Grooved Substrates"
Appl.
Phys. Lett. 64 (4), 472-474 (1994).
ABSTRACT:
GaAs trench-buried quantum wires were fabricated by using V-grooved AlAs
trenches grown on V-grooved (001) substrates. These trench structures with
vertical (110) sidewalls were formed by the faceting of (110) planes, and
lateral growth of these planes reduced the trench width to less than 20 nm. A
cross-sectional scanning electron microscope image of these trench-buried
structures showed GaAs wires about 20 nm wide and 20 nm thick. The growth of
these wires is enhanced by the capture of Ga species into the trenches.
Blueshifts and strong anisotropy of photoluminescence confirm two-dimensional
quantum confinement.
115. L. C. Su, I. H. Ho, N.
Kobayashi, and G. B. Stringfellow
"Order-Disorder
Heterostructure In Ga0.5in0.5p With Delta-E(G)=160 Mev"
J.
Cryst. Growth 145 (1-4), 140-146 (1994).
ABSTRACT:
Ordering in Ga0.5In0.5P can be controlled by variations in the substrate
temperature during organometallic vapor phase epitaxial (OMVPE) growth. Growth
at 720 degrees C at a rate of 0.5 mu m/h is shown to produce completely
disordered material, as evidenced by the transmission electron diffraction
(TED) and the photoluminescene (PL) results. The ordering produced at a growth
temperature of 620 degrees C is found to depend strongly on the substrate
misorientation, Transmission electron micrographs and TED patterns for misorientations
of 0 degrees, 3 degrees, 6 degrees, and 9 degrees from (001) toward the [110]
direction in the lattice show that increasing the misorientation from 0 degrees
to 3 degrees leads to the elimination of one variant, the elimination of twin
boundaries, and an overall increase in the degree of order. Further increases
in the misorientation angle to 6 degrees and 9 degrees at this growth
temperature lead to increasing disorder, although only one variant is formed
and the distance between antiphase boundaries (APBs) increases monotonically
with increasing theta(m). This wide variation in ordering behavior has allowed
the growth of an order/disorder heterostructure for a substrate misorientation
of 3 degrees. The heterostructure consists of a Ga0.52In0.48P layer 0.5 mu m
thick grown at 740 degrees C followed by an ordered layer 0.4 mu m thick grown
at 620 degrees C. The X-ray diffraction results show that both layers are
precisely lattice-matched to the GaAs substrate. TED patterns show that the
first layer is completely disordered and the top layer is highly ordered, with
only a single variant. High resolution images indicate that the interface is
abrupt, with no dislocations or other defects. 10 K PL shows two sharp and
distinct peaks at 1.995 and 1.830 eV for high excitation intensities. The peak
separation is even larger at lower excitation intensities. The two peaks come
from the disordered and ordered material, respectively. The peak separation
represents the largest energy difference between ordered and disordered
material reported to date. This large energy difference, 6.6kT at room
temperature, may make such heterostructures useful for photonic devices such as
light emitting diodes, lasers, and solar cells.
116. H. Tabei, M. Takahashi, S.
Hoshino, O. Niwa, and T. Horiuchi
"Subfemtomole
Detection Of Catecholamine With Interdigitated Array Carbon Microelectrodes In
Hplc"
Anal.
Chem. 66 (20), 3500-3502 (1994).
ABSTRACT: An
IDA carbon microelectrode for HPLC was fabricated by photolithographic
techniques from the carbon film of pyrolyzed 3,4,9,10-perylenetetracarboxylic
dianhydride on thermally oxidized silicon wafers. The IDA electrode consisted
of 300 pairs, the finger widths and gaps were 5 mu m, and each finger was 2 mm
long. The electrode in a small-volume thin-layer cell incorporated in a
microbore HPLC system achieved a low detection limit for dopamine due to
current enhancement by redox cycling and low background noise at the carbon IDA
microelectrode. The detection Limit of 0.5 fmol of dopamine can be realized
because of the low noise level and high current density.
117. A. Taguchi, K. Takahei,
and Y. Horikoshi
"Multiphonon-Assisted
Energy-Transfer Between Yb 4f Shell And Inp Host"
J.
Appl. Phys. 76 (11), 7288-7295 (1994).
ABSTRACT:
118. K. Takahei and A. Taguchi
"Efficient
Er Luminescence-Centers Formed In Gaas By Metalorganic
Chemical-Vapor-Deposition With Oxygen Codoping"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 33
(1B), 709-711 (1994).
ABSTRACT:
Er-doped GaAs is grown by low-pressure metalorganic chemical vapor deposition
with and without oxygen codoping. Optically efficient Er-oxygen complex centers
are formed when a small amount of oxygen is present in the growth atmosphere.
In situ monitoring of the surface morphology by light scattering from the
growing surface with and without oxygen codoping suggests that migration of Er
atoms on the surface is pinned by the formation of an Er-oxygen complex. We
speculate that this effect suppresses the formation of Er-rich clusters and
allows the formation of a high concentration of uniformly dispersed Er-oxygen
complex centers that have a high luminescence efficiency.
119. K. Takahei, A. Taguchi, Y.
Horikoshi, and J. Nakata
"Atomic
Configuration Of The Er-O Luminescence Center In Er-Doped Gaas With Oxygen
Codoping"
J.
Appl. Phys. 76 (7), 4332-4339 (1994).
ABSTRACT:
This article investigates the structure of an Er luminescence center in GaAs by
using its intra-4f-shell luminescence spectrum as an atomic probe to identify
the atomic configuration. This Er center is formed in GaAs by metalorganic
chemical vapor deposition with O codoping and the center shows a high
efficiency and a sharp luminescence spectrum under above-band-gap
photoexcitation. A single luminescence line in the spectrum of a GaAs:Er,O
splits into more than eight lines in the spectrum of Al0.01Ga0.99As:Er,O. This
drastic change due to the addition of 1% Al can be explained by assuming that,
because of the high tendency of Al atoms to react with O atoms, the Al atoms
preferentially occupy the nearest-neighbor Ga sites of two O atoms, both of
which are coupled with the Er atom. Based on the luminescence spectra and
additional experiments of Rutherford backscattering and secondary ion mass
spectroscopy, we propose that the structure of the Er luminescence center under
study is Er occupying the Ga sublattice with two O atoms most likely located at
the nearest-neighbor As sites. An Er-related spectrum of GaAs0.97P0.03:Er,O can
also be understood based on this model if the chemical difference of Al and P
is taken into account.
120. H. Takayanagi, J. B.
Hansen, and J. Nitta
"Mesoscopic
Fluctuations In The Critical-Current In Inas-Coupled Josephson-Junctions"
Physica
B 203 (3-4), 291-297 (1994).
ABSTRACT:
Mesoscopic fluctuations were confirmed for the critical current in a p-type
InAs-coupIed Josephson junction. The critical current was measured as a
function of the gate voltage corresponding to the change in the Fermi energy.
The critical current showed a mesoscopic fluctuation and its behavior was the
same as that of the conductance measured at the same time in both the weak and
strong localization regimes. The magnitude and the typical period of the
fluctuation are discussed and compared to theoretical predictions.
121. K. Takeda
"Electronic-Structure
Of Random Copolymers"
J.
Math. Chem. 15 (3-4), 323-337 (1994).
ABSTRACT: The
electronic structure of random copolymers (RCP) is theoretically investigated
by the single-site coherent potential approximation. The results are also
compared with those by the band calculation for the corresponding ordered
system. In the A1-xBx binary RCP, a strong reduction in the system band gap
(E(g)(A1-xBx)) is found in the dilute B region when the system has the relation
of E(g)(A) > E(g)(B). This dependence is caused by the asymmetric quenching
in the density-of-states (DOS) singularity at the band-edge states. The
gap-opening mechanism and the asymmetric quenching are discussed by focusing on
the role of the spatial dimension on the electronic structure of the random
system, and the theoretical treatment is finally applied to the calculation of
the joint DOS for the Si-Ge RCP system.
122. K. Takeda and K. Shiraishi
"Theoretical
Possibility Of Stage Corrugation In Si And Ge Analogs Of Graphite"
Phys.
Rev. B 50 (20), 14916-14922 (1994).
ABSTRACT:
123. K. Takeda, K. Shiraishi,
M. Fujiki, M. Kondo, and K. Morigaki
"Photocreated
Metastable States In Polysilanes"
Phys.
Rev. B 50 (8), 5171-5179 (1994).
ABSTRACT:
Photocreated metastable states in organopolysilane (PSi) solids are observed
using the electron-spin-resonance (ESR) technique. Two types of light-induced
ESR (LESR) spectra are found depending on the excitation photon energy. These
two types of LESR centers are annihilated by thermal annealing. Based on a
first-principle electronic calculation, the origins of these LESR centers have
been discussed. The lowest photoexcitation (approximately 3.5 eV) in PSi
induces the Si skeleton stretching forces, which creates a weak bond (WB) in
several places of the Si skeleton. Electronically, this WB acts as a
self-trapping center for the photoexcited sigma electron. The other higher
photoexcitation (over 4.8 eV) causes side-pendant dissociation, which creates a
dangling bond (DB) and causes the localized midgap state. The four lines found
in the higher-energy excitation are considered to arise from hyperfine
interaction between this DB electron and a sodium impurity nucleus.
124. K. Takei, D. J. Rogers,
and Y. Maeda
"Bias
Effect On Compositional Separation In Sputtered Co-Cr Films"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 33
(10), 5739-5742 (1994).
ABSTRACT: The
effect of de substrate bias on compositional separation (CS) in sputtered Co-Cr
films is examined using spin-echo Co-59 NMR and transmission electron
microscopy. It is observed that the degree of CS decreases monotonically with
increasing negative bias voltage. Slight positive bias voltage, however, is
found to enhance CS, resulting in increased saturation magnetization and a
higher anisotropy field. The elimination of Ar ion bombardment at the film
surface during deposition is thought to be effective in enhancing CS.
125. K. Takei, D. J. Rogers,
and Y. Maeda
"Nmr-Study
Of Magnetic And Compositional Inhomogeneities In Co-Cr Thin-Films"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 33
(2), 1027-1028 (1994).
ABSTRACT:
Spin-echo Co-59 NMR is employed to detect magnetically distinct components in a
Co-Cr thin film. Magnetic components with different values of the anisotropy
field can be detected by measuring spin-echo intensity as a function of rf
pulse field applied to the sample. For a film deposited at 400-degrees-C, two
magnetic components are observed. The chemical composition is estimated for
each component from the NMR frequency spectra.
126. K. Takei, J. Suzuki, Y.
Maeda, and Y. Morii
"Micromagnetic
Domain Observations Of Co-Cr Films By Neutron-Scattering"
IEEE
Trans. Magn. 30 (6), 4029-4031 (1994).
ABSTRACT:
Magnetic microstructures revealed by neutron small angle scattering are
correlated with the compositional separation (CS) in sputtered Co-22at%Cr thin
films for. high density magnetic recording. The CS is confirmed to be strongest
for deposition temperatures from 150 degrees C to 400 degrees C, using nuclear
magnetic resonance. The finest magnetic particles, less than 10 mm in diameter,
are detected in a film deposited at 200 degrees C, in good agreement with the
smallest features observed in the etched microstructure by transmission
electron microscopy. This indicates that CS produces magnetic grains much
smaller than the crystal grains which can, therefore, de applied to synthesize
Co-Cr thin film media for ultra high density magnetic recording.
127. Y. Tanaka, A. Hasegawa,
and H. Takayanagi
"Tunneling
Conductance Of A Quantum-Dot Formed By A Super-Conducting Pari Potential"
Physica
B 194, 1761-1762 (1994).
ABSTRACT: The
tunneling conductance of the quasiparticle of a quantum dot structure, which is
a normal region surrounded by a superconducting pair potential, is obtained
under a magnetic field weaker than the lower critical field of the
superconductor. It strongly depends on the number of the magentic flux quanta
that penetrates the normal dot region.
128. S. Tarucha, T. Honda, T.
Saku, and Y. Tokura
"Charging
Effects In Small-Area Modulation-Doped Double-Barrier Heterostructures"
Surf.
Sci. 305 (1-3), 547-552 (1994).
ABSTRACT:
Charging effects on resonant tunneling are studied in modulation-doped
double-barrier heterostructures. We observe a blockade of the tunneling current
around zero-bias in small-area devices, while in large-area devices we observe
a tunneling current with a zero-threshold bias due to the modulation doping.
The blockade voltage width varies in proportion to the inverse square of the
conducting diameter, and agrees well with the calculated charging energy for a
single electron. At the high voltage end of this blockade region we observe
step-like current-voltage features and fine structure in the form of small
peaks and shoulders. This fine structure is related to the interplay between
charging and size quantization effects.
129. H. Teramae and J. Michl
"Electronic
States Of Linear Tetrasilane And Polysilanes"
Mol.
Cryst. Liq. Cryst. Sci. Technol. Sect. A-Mol. Cryst. Liq. Cryst. 256,
149-159 (1994).
ABSTRACT: The
standard Sandorfy C model of electronic structure of polysilanes is inherently
incapable of providing a physical interpretation of the observed conformational
effects on UV spectra. We describe a more complicated ladder C model, which
still considers only the two backbone hybrid orbitals on each silicon atom, but
includes the transfer integrals between all pairs of orbitals on a pair of
neighboring silicons. Already at the Huckel level, this model accounts for the
general features of the observed spectra both as a function of chain length and
of conformation. Results of our ab initio calculations suggest, however, that
for general non-planar conformations the backbone orbitals should not be
treated separately from those that carry the substituents, at least not in
relatively short chains. The simplest level at which the conformational effects
on the spectra of oligosilanes of all lengths can be accounted for
simultaneously will probably be the even more complicated ladder H model, in
which all four valence orbitals of each silicon and one orbital of each
substituent are considered explicitly.
130. Y. Tokura and S. Tarucha
"Exchange
Interaction In Quantum-Wire Subbands"
Phys.
Rev. B 50 (15), 10981-10989 (1994).
ABSTRACT: The
many-electron ground state is studied in a quantum wire with several populated
spin and orbital subbands. The many-body effect is treated in the lowest order.
The phase diagram of the subband population is obtained as a function of
magnetic field and the strength of the confining potential. If the magnetic
field is small, there is a phase boundary between spin-polarized states and
partially spin-polarized states. Using these results, transport characteristics
are calculated using Landauer's formula and a dip is predicted in the
conductance plateau of 2e(2)/h.
131. Y. Tomioka, M. Naito, K.
Kishio, and K. Kitazawa
"The
Meissner And Shielding Effects Of High-Temperature Oxide Superconductors"
Physica
C 223 (3-4), 347-360 (1994).
ABSTRACT: The
Meissner and shielding effects were investigated systematically on single
crystals of (La1-xSrx)2CuO4, YBa2Cu3O7 and Bi2Sr1.8CaCu2O8. Significant
differences in the low-temperature Meissner fraction (f(M)) in the same
materials observed under various fields and sample sizes, were explained
consistently and quantitatively, based on the vortex-pinning model. Extending
the model employed, the pinning critical current could be estimated as a
function of T from the set of the shielding and Meissner curves. The Meissner and
shielding effects in the polycrystalline samples were also measured in a
similarly systematic manner and could be interpreted by considering the
effective sample size of the polycrystals, showing a cross-over of this
quantity from the grain size at high fields to macroscopic sample size at low
fields.
132. M. Tsukada, A. Misawa, J.
Nishikido, Y. Shimazu, and H. Nakano
"Experiments
On Photonic Cell Switching With An Optical Input Buffer"
Electron.
Lett. 30 (13), 1081-1082 (1994).
ABSTRACT: The
authors describe photonic cell switching experiments using an optical input
buffer. The buffer controls cell throughput to a switch module according to
back-pressure signals from a switch controller. The buffer has a size of three
cells consisting of two kinds of fibre delay line. The optical cells are
switched to dual ports through the optical buffer. Buffering and switching
experiments are performed for 2.5Gbit/s 64bit optical cells, and the bit error
rate is measured.
133. M. Ueda and T. Ando
"Effects
Of Barrier Traversal Time On Escape Rate Through A Small-Capacitance Tunnel
Junction"
Superlattices
Microstruct. 16 (3), 279-281 (1994).
ABSTRACT:
This paper describes self-consistent determination of the
transfer-energy-dependent escape rate and barrier traversal time of electrons
under the influence of the electromagnetic environment. This rate lets us
examine dissipative and nondissipative tunneling rate separately and its
integral over the transfer energy gives the total escape rate that is obtained
by the instanton technique. It is found that the escape rate is exponentially
enhanced as the capacitance of the junction is reduced.
134. M. Ueda and T. Ando
"Potential
Renormalization In Mesoscopic Tunneling - Reply"
Phys.
Rev. Lett. 73 (20), 2785-2785 (1994).
ABSTRACT:
135. M. Ueda and T. Ando
"Transfer-Energy-Dependent
Escape Rate Of Electrons Through A Small-Capacitance Tunnel Junction"
Phys.
Rev. B 50 (11), 7820-7832 (1994).
ABSTRACT: The
dynamics of a tunneling electron through a small-capacitance tunnel junction
are studied by developing a method for self-consistently determining escape
rate and barrier traversal time for those electrons that transfer a given
energy to the electromagnetic environment. The transfer-energy-dependent escape
rate lets us examine dissipative and nondissipative tunneling rates separately
and its integral over the transfer energy gives the total escape rate that is
obtained by the instanton technique. It is found that the escape rate increases
exponentially with increasing the ratio of the elementary charging energy to
the quantized energy of the environment, but that the traversal time peaks at
one particular ratio. As the frequency of the electromagnetic mode increases,
an effective potential is shown to change from linear (dominated by the
zero-point fluctuations of charge on the junction) to parabolic (dominated by
the static polarization of the charge). Possible experimental situations for
observing the predicted effects are discussed.
136. M. Ueda and T. Ando
"Electron-Escape
Rate And Barrier Traversal Time Influenced By The Electromagnetic
Environment"
Phys.
Rev. Lett. 72 (11), 1726-1729 (1994).
ABSTRACT:
Self-consistent determination of electron escape rate and barrier traversal
time under the influence of the electromagnetic environment reveals that the
escape rate increases monotonically with increasing ratio of the elementary
charging energy to the barrier height but that the traversal time peaks at one
certain ratio. As the frequency of the electromagnetic mode increases, an
effective potential for a tunneling electron changes from linear to parabolic,
dominated, respectively, by the zero-point fluctuations of the charge on the
junction and its static polarization. Possible experimental situations for
observing these predictions are discussed.
137. M. Ueda and N. Imoto
"Anomalous
Commutation Relation And Modified Spontaneous Emission Inside A
Microcavity"
Phys.
Rev. A 50 (1), 89-92 (1994).
ABSTRACT:
Usual quantum-optical operator relations for a beam splitter are shown to lead
to an anomalous commutation relation inside a microcavity. The physical origin
of this anomaly is identified as self-interference of the mode whose coherence
length is longer than the round-trip length of the cavity. Altered spontaneous
emission of an excited atom is found to be a direct manifestation of this
anomalous commutation relation. The anomalous Heisenberg uncertainty relations,
which are derived from the commutation relation according to the Schwartz
inequality, cannot be detected by probing the internal field with a beam
splitter. The anomalous commutation relation, however, can be related to the
change in the effective reflectivity of the beam splitter. The similarity and
difference between an excited atom and a probe beam splitter are discussed.
138. K. Y. Uomori and S. Y.
Nishida
"The
Dynamics Of The Visual-System In Combining Conflicted Kde And Binocular
Stereopsis Cues"
Percept.
Psychophys. 55 (5), 526-536 (1994).
ABSTRACT: The
dynamics of the visual system in combining multiple depth cues were
investigated by measuring the temporal change in the perceived 3-D shape of a
random-dot stimulus with conflicting kinetic depth effect (KDE) and binocular
stereopsis cues. The KDE shape perception dominated for the first few seconds,
and then was gradually supplanted by the stereo shape perception. The effects
of various pre-adaptation stimuli suggested that the temporal change in the
perceived shape resulted from a self-adaptation of the KDE mechanism that
occurs mainly at the levels of motion and relative motion detection.
139. K. Uwai and N. Kobayashi
"Real-Time
Observation Of Surface Dielectric Responses Of Gaas(001) Using Surface
Photoabsorption"
Appl.
Surf. Sci. 82-3, 290-297 (1994).
ABSTRACT:
Surface photo-absorption is used to observe the changes in isotropic and
anisotropic surface dielectric responses caused by As desorption during surface
conversion from c(4 x 4) to (2 x 4) gamma of As-stabilized GaAs(001) surfaces.
The anisotropic part agrees with the change in the surface dielectric
anisotropy spectrum observed in reflectance-difference measurements during this
surface conversion. The spectral evolutions of surface dielectric response are
observed in real time with a time resolution of 0.1 s during surface
conversion.
140. K. Uwai and N. Kobayashi
"Dielectric
Response Of As-Stabilized Gaas-Surfaces Observed By Surface
Photoabsorption"
Appl.
Phys. Lett. 65 (2), 150-152 (1994).
ABSTRACT:
This letter discusses changes in the isotropic and anisotropic surface
dielectric response caused by surface conversion from c(4x4) to (2X4) of a
GaAs(001) As-stabilized surface, observed using surface photo-absorption. The
anisotropic part quantitatively reproduces the change in the surface dielectric
anisotropy spectra observed in reflectance difference measurements during this
surface conversion. The isotropic part can be measured only by surface
photo-absorption and comparison is made with a calculation using a three-phase
model consisting of vacuum/As/GaAs.
141. L. M. Weegels, T. Saitoh,
and H. Kanbe
"Real-Time
Investigations Of Gaas Surface Cleaning With A Hydrogen
Electron-Cyclotron-Resonance Plasma By Optical Reflection Spectroscopy"
Appl.
Phys. Lett. 65 (24), 3117-3119 (1994).
ABSTRACT:
142. L. M. Weegels, T. Saitoh,
H. Oohashi, and H. Kanbe
"In-Situ
Monitoring Of Electron-Cyclotron-Resonance Plasma Processing Of Gaas-Surfaces
By Optical Reflection Spectroscopy"
Appl.
Phys. Lett. 64 (20), 2661-2663 (1994).
ABSTRACT: In
situ reflection spectroscopy is demonstrated to be a useful technique for
monitoring the damage to the surface of GaAs substrates induced by ions from an
electron cyclotron plasma. Distinct differences in the reflectance spectra of GaAs
substrates are observed between etching by argon ions and chemical cleaning by
hydrogen ions. For argon it is found that the damage layer thickness increases
linearly with the argon ion energy. Hydrogen ions induce a damage layer of 3.1
nm and arsenic atoms are preferentially removed from the surface as the ion
energy increased.
143. S. Yamada, K. Maezawa, W.
T. Yuen, and R. A. Stradling
"X-Conduction
2-Dimensional Subband Structure And Order In Algaas/Alas Quantum-Wells"
Physica
B 201, 295-300 (1994).
ABSTRACT: The
subband structure of two-dimensional X-band electrons in modulation-doped very
thin (25-75 angstrom) AlAs quantum wells was studied in magnetotransport
experiments and analyzed in self-consistent calculations. Effective mass
estimation based on temperature dependent magnetoresistances clearly showed
X(z) - X(xy) crossover at an AlAs thickness of about 45 angstrom, which is much
less than the crossover thickness in AlAs/GaAs type II superlattices (60
angstrom). Considering the results of self-consistent calculations together
with some observed anomalies in X(xy) electron magnetoresistances, we can
conclude that this difference is due to the effect of doping and to the
degeneracy change in k-space occurring at the crossover thickness of AlAs.
144. S. Yamada, K. Maezawa, W.
T. Yuen, and R. A. Stradling
"X-Conduction-Electron
Transport In Very Thin Alas Quantum-Wells"
Phys.
Rev. B 49 (3), 2189-2192 (1994).
ABSTRACT:
Magnetotransport behavior of two-dimensional X-band electrons created in modulation-doped
very thin (25-75 Angstrom) AlAs quantum wells was studied. Effective-mass
analysis based on temperature-dependent magnetoresistances clearly showed
X(z)-X(xy) crossover at an AlAs thickness of about 45 Angstrom. This value is
much smaller than that in an AlAs/GaAs type-II superlattice (60 Angstrom).
Origins of this difference were discussed in terms of the effect of doping and
degeneracy change and of the change of strain due to the structure difference.
145. T. Yamada and Y. Horikoshi
"Comparison
Of Gaas Facet Formation On Patterned Substrate During Molecular-Beam Epitaxy
And Migration-Enhanced Epitaxy"
Jpn.
J. Appl. Phys. Part 2 - Lett. 33 (7B), L1027-L1030 (1994).
ABSTRACT: We
compare the film thickness profile and facet formation of GaAs films grown on a
patterned substrate by migration-enhanced epitaxy (MEE) and by molecular beam
epitaxy (MBE). The film thickness profile indicates that the Ga diffusion
length during MBE growth decreases as the As pressure increases. In contrast, the
diffusion length during MEE growth is independent of the As pressure. The
facets resulting from MBE and MEE diff er greatly. The dominant facet produced
by MBE is in the (111)B plane, whereas (110), (113)B and (221)B are the most
observable facet planes resulting from MEE. From these results, it is found
that Ga atoms migrate to occupy every available site on each plane, with excess
atoms moving to other index planes in MEE growth.
146. T. Yamada, K. Kinoshita,
and H. Shibata
"Synthesis
Of Superconducting T'-(La1-Xcex)(2)Cuo4"
Jpn.
J. Appl. Phys. Part 2 - Lett. 33 (2A), L168-L169 (1994).
ABSTRACT: A
new preparation method far obtaining superconducting T'-(La1-xCex)(2)CuO4 is
presented. The method consists of three processes: precursor material synthesis,
oxidation and T'-phase formation. The single phase has been obtained for 0.065
less than or equal to x less than or equal to 0.08. The maximum superconducting
onset (T-c(onset)) and zero-resistance (T-c (zero)) temperatures are 30 K and
17 K, respectively, which are obtained when x=0.065. The T-c(onset) obtained
here is higher than those of other T'-type cuprates.
147. H. Yamaguchi, Y. Homma,
and Y. Horikoshi
"In-Situ
Monitoring Of 1st-Order Phase-Transition On Inas(001) Surfaces By Scanning
Electron Surface Microscopy"
Appl.
Surf. Sci. 82-3, 223-227 (1994).
ABSTRACT:
Domain formation during the phase transition on an InAs(001) surface under As
pressure was observed directly for the first time by using scanning electron
surface microscopy, which is a surface-sensitive scanning electron microscopy
technique. Detailed analysis also verified that the role of step edges during
transition differs between As-atom desorption and adsorption.
148. H. Yamaguchi and Y.
Horikoshi
"Unified
Model For Structure Transition And Electrical-Properties Of Inas (001) Surfaces
Studied By Scanning-Tunneling-Microscopy"
Jpn.
J. Appl. Phys. Part 2 - Lett. 33 (10A), L1423-L1426 (1994).
ABSTRACT:
Thermal stability of the (2x4) structures on InAs and GaAs (001) surfaces is
studied by using scanning tunneling microscopy with atomic resolution. Even
just before the transition to a (4x2) structure, the annealed InAs surface has
much lower density of kinks in the dimer vacancy rows than the annealed GaAs.
This difference leads to a unified model that can explain both the 1st order
phase transition and the peculiar electric properties of an InAs (001) surface.
149. H. Yamaguchi and Y. Horikoshi
"Arsenic
Pressure-Dependence Of 1st-Order Phase-Transition On Inas (001) Surface"
Appl.
Phys. Lett. 64 (19), 2572-2574 (1994).
ABSTRACT: The
role of As pressure in the first-order phase transition between As-covered
(2X4) and In-covered (4X2) structures on InAs (001) surfaces is investigated
using reflection high-energy electron diffraction. The dependence of transition
temperatures on As pressure is well explained by Monte Carlo simulation with a
two-dimensional lattice gas model, and the interaction energy is quantitatively
obtained. The influence of metastability on As desorption is also clarified by
comparing the experiments and simulations.
150. H. Yamaguchi and Y.
Horikoshi
"Step
Motion And Structure Transition On Inas And Gaas (001) Surfaces Observed By
Scanning-Tunneling-Microscopy"
Jpn.
J. Appl. Phys. Part 1 - Regul. Pap. Short Notes Rev. Pap. 33
(1B), 716-720 (1994).
ABSTRACT: The
step motion and structure transition on InAs and GaAs (001) surfaces are
directly observed by scanning tunneling microscopy at high temperatures. A
stable (2x4) structure is observed for the InAs surface even at temperatures
high enough to cause the motion of monomolecular steps and kinks. At higher
temperatures, domains with an In stable (4x2) Structure (As desorbed region)
are clearly observed surrounded by As stable (2x4) structures. These results
differ from those for GaAs surfaces and indicate strong lateral interaction in
(2x4) structures on InAs.
151. R. Yano, M. Mitsunaga, N.
Uesugi, and M. Shimizu
"Temperature-Dependence
Of The Homogeneous Width Of Eu(3+) Spectral-Lines In Silicate Glass Measured By
Accumulated Photon-Echoes"
Phys.
Rev. B 50 (13), 9031-9034 (1994).
ABSTRACT: The
temperature-dependent homogeneous width of the 5D(0)-7F(0) transition of Eu3+
in a pure silicate glass fiber has been measured by accumulated photon echoes
between 1.6 and 44 K. The temperature dependence of the homogeneous width shows
a crossover from T-linear (T < 7 K) to T2 (T > 7 K). The whole
temperature dependence of the homogeneous width between 1.6 and 44 K can be
explained by the configurational changes of the glass which is modeled by
two-level systems (TLS's) and a Raman process involving low-frequency
vibrational modes of the silicate glass (the rotations of SiO4 tetrahedra). The
T-linear temperature dependence is attributed to the TLS process. The anomalous
T2 dependence down to 10 K cannot be explained by only one process, but can be
explained by the contributions of both the TLS process and the Raman process.
Above 40 K, the Raman process becomes the dominant dephasing mechanism.
152. J. Yumoto, K. W. Delong,
and N. Uesugi
"Coherent
Transients In Cdsse Microcrystallites Doped In Glasses"
Phys.
Rev. B 49 (16), 11322-11326 (1994).
ABSTRACT:
Coherent transient effects, in CdSSe microcrystallites are observed by a
pump-probe measurement. The probe transmission shows oscillatory structures in
the temporal and spectral domains when the probe reaches the sample before the
pump. This oscillation is attributed to the photon echo propagating in the
direction of the probe. The A-B splitting of the valence sublevel in CdSSe
microcrystallites hidden in the wide inhomogeneous broadening can be resolved
using the polarization dependence of the transitions from A and B valence
sublevels to the conduction sublevel.