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3. High Technology - Vol. 42
Advanced Electronic Technologies and Systems Based on Low-Dimensional Quantum Devices
edited by
Minko Balkanski Universite Pierre et Marie Curie, Paris, France
and
Nikolai Andreev Technical University of Sofia, Sofia, Bulgaria
Springer-Science+Business Media, BV
Proceedings of the NATO Advanced Study Instute on Advanced Electronic Technologies and Systems Based on Low-Dimensional Quantum Devices Sozopol, Bulgaria 18-28 September 1996
A C.I.P. Catalogue record for this book is available from the Library of Congress.
ISBN 978-90-481-4964-3 ISBN 978-94-015-8965-9 (eBook) DOI 10.1007/978-94-015-8965-9
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Softcover reprint of the hardcover 1 st edition 1997
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TABLE OF CONTENTS
Preface
Acknowledgments
1. Fnndamentals on Quantum Structures for Electro-Optical
Devices and Systems
1.1 Electron State Symmetries and Optical Selection Rilles in the
(GaAs)m(AIAs)n Superlattices Grown Along the [001], [110], and [111]
Directions.
Yu. E. Kitaev, A. G. Panfilov, P. TroncandR. A. Evarestov
1.1.1 Electronic Structure of AlAs/GaAs Superlattices with an
Embedded Centered GaAs Quantum Well.
V. Donchev, Tzv. Ivanov andK. Gennanova
1.1.2 Electronic States in Graded Composition Quantum Wells under a
Constant Electric Field.
S. Vlaev, A. Miteva and V. Don<.:hev
1.1.3 Dimension Related Effects on the Structure Perfection in Si/SiC
Milltilayer Structures.
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51
55
E. Valcheva, T. Paskova, O. Kordina, R. Yakimova, E. Janzen 59
1.1.4 Effect of the Non-Parabolicity and Dynamical Screening on the
Second-Hannonic Generation in Doubly Resonant Asymmetric
Quantum Well Structures.
M. Zaluzny and V. Bondarenko 63
1.1.5 Optical Diagnostics of Quantum Dots in GaAsIlnxGal_xAs
Heterostructures.
V. Ya. Aleshkin, V. M. Danil'tsev, O. I. Khrykin, Z. F.
Krasil'nik, D. G. Revin, V. I. Shashkin 65
1.1.6 Generation of High - Frequency Oscillations by Electromagnetic
VI
Shock Wave (EMSW) in Nonlinear Transmission lines on the Basis of
Multilayer Heterostructures.
A. B. Kozyrev and A. M. Belyantsev 67
1.1.7 Picosecond Spectroscopy Studies of CuS and CuInS2 Quantum
Dots with Chemically Modified Surface.
A. M. Malyarevich, K. V. Yumashev, P. V. Prokoshin, M. V.
Artemyev, V. S. GurinandV. P. Mikhailov
1.1.8 Intensity Induced Polarization Rotation due to Cascading in
ImbalancedType II Nearly Phase Matched Frequency Doubling.
69
S. Saltiel, I. Buchvarov, K. Koynov, P. Tzankov and Ch. Iglev 71
1.2 Modeling Quantum Well Laser Diode Structures.
P. Blood, D.L. Foulger and P.M. Smowton 77
1.2.1 Silicium Crystal Photoluminescence as Transducer for
Biosensors.
N. F. Starodub, L. L. Fedorenko, V. M. Starodub, S. P. Dikij 91
1.2.2 Injection Lasers based on Vertically Coupled Quantum Dots.
A. E. Zhukov, V. M. Ustinov, A. Yu. Egorov, A. R. Kovsh,
N. N. Ledentsov, M. V. Maksimov, A. F. Tsatsul'nikov, N.
Yu. Gordeev, S. V. Zaitsev, P. S. Kop'ev.
1.2.3 Infrared Emission of Hot Holes in Strained Multi-Quantum
Well Heterostructures InGaAs/GaAs under Real Space Transfer.
V. Ya. Aleshkin, A. A. Andmnov, A. V. Antonov, N. A.
Bekin, V. I. Gavrilenko, D. G. Revin, E. R. Lin'kova, I. G.
93
Matkina, E. A. Uskova andB. N. Zvonkov 97
1.3 Microcavity Semiconductor Lasers
J. G. McInerney, Damien P. Courtney, Peter M. W. Skovgaard arrl
Brian Corbett 99
2. MQW Optoelectronic Devices and Systems
2.1 Exciton Absorption Saturation and Camer Transport in Quantum
Well Semiconductors.
A. Miller, T. M. Holden, G. T. Kennedy, A. R. Cameron and P.
VII
Riblet 117
2.2. IntegratedOptoelectronics - the Next Technological Revolution.
A.S. Popov 137
2.3. Opportunities of Vertical - Cavity - Surface - Emitting Lasers
(VCSEL) in display and optical communication systems.
A.S. Popov 155
2.4. New Integrated Photoreceiver Systems - Charge Coupled Devices
(CCD).
A.S.Popov 175
2.5. Optical Switches and Modulators for Integrated Optoelectronic
Systems.
A.S.Popov 189
2.5.1 Scalar Off-Resonant Modulation Instabilities in Genernl
Rare-Earth Doped Fiber Amplifying Devices.
T. Mirtchev 201
2.5.2 Quantum Dot Laser With High Temperature Stability of
Threshold Current Density.
A.R. Kovsh, A.E. Zhukov, M.A. Odnoblyudov, A. Yu.
Egorov, Y.M. Ustinov, N.N. Ledentsov, M.Y. Maksimov,
A.F. Tsatsul'nikov, N. Yu. Gordeev, S.Y. Zaitsev and P.S.
Kop'ev 207
VJ1l
3. Soliton-Based Switching, Gating and Transmission
Systems
3.1 Soliton-Based Logic Gates and Soliton Transmission Systems.
A. D. Boardman,R. Putman andK. Xie 209
3.1.1 100 GHz * 100 km Optical Soliton Data Transmission
System, Basedon Gradient Distributed Er3+ - Doped Fiber Amplifiers.
T. Mirtchev 267
3.1.2 Control of Lightguiding in H:LiTa03 and H:LiNb03 Thin
Films.
C. C. Ziling, V. V. Atuchin, I. Savatinova, S. Tonchev, M. N.
Armenise and V. N. Passaro 277
3.1.3 Self - Phase Modulation due to Third-Order Cascading:
Application to All-Optical Switching Devices.
S. Tanev,K. Koynov, S. Saltiel, K. XieandA. D. Boardman 281
Index 289
NA TO ASI held in Sozopol, Bulgaria, September 18-28, 1996
ADVANCED ELECTRONIC TECHNOLOGIES AND SYSTEMS BASED
ON LOW -DIMENSIONAL QUANTUM DEVICES
Sponsored by
NATO Scientific and Environmental Affairs Division
Ministere de I 'Enseignement Superieur et de la Recherche, France
Universite Pierre et Marie Curie, Paris, France
University St. Kliment Ohridski, Sofia, Bulgaria
Technical University, Sofia, Bulgaria
Institut des Hautes Etudes pour Ie development de la Culture, de la Science et
de la Technologie en Bulgarie, Paris, France.
Principal School Support NATO Program for Priority on High Technology
Bulbank, Bulgarian Bank for Foreign Trade, Sofia, Bulgaria
Universite Pierre et Marie Curie, Paris, France
IX
PREFACE
This volume on Advanced Electronic Technologies and Systems based on Low
Dimensional Quantum Devices closes a three years series of NATO - AS!' s.
The first year was focused on the fundamental properties and applications. The second year
was devoted to Devices Based on Low-Dimensional Semiconductor Structures. The third year is
covering Systems Based on Low-Dimensional Quantum Semiconductor Devices.
The three volumes containing the lectures given at the three successive NATO - ASI's
constitute a complete review on the latest advances in semiconductor Science and Technology
from the methods of fabrication of the quantum structures through the fundamental physics am basic knowledge of properties and projection of performances to the technology of devices and
systems.
In the first volume: " Fabrication, Properties and Application of Low Dimensional
Semiconductors" are described the practical ways in which quantum structures are produced, the
present status of the technology, difficulties encountered, and advances to be expected. The basic
theory of Quantum Wells, Double Quantum Wells and Superlattices is introduced and the
fundamental aspects of their optical properties are presented. The effect of reduction of
dimensionality on lattice dynamics of quantum structures is also discussed.
In the second volume: " Devices Based on Low Dimensional Structures" the fundamentals
of quantum structures and devices in the two major fields: Electro-Optical Devices and
Pseudomorphic High Eectron Mobility Transistors are extensively discussed.
Xl
Xll
In the third volume: " Advanced Electronics Technology and Systems Based on Low -
Dimensional Quantum devices ", which we present now, the major developments in Quantum
Structures Systems are discussed in three main chapters:
Fundamentals on Quantum Structures for Electro-Optical Devices and Systems
MQW Optoelectronic Devices and Systems
Soliton-Based Switching, Gating and Transmission Systems
Fundamentals on Quantum Structures for Electro-Optical Devices and Systems
As an example of the recent development in basic research the first chapter is devoted to
Electron State Symmetries and Optical Selection Rules in the (GaAs)m(AIAs)n Superlattices
Grown Along the [001], [110], and [111] Directions. Using the method of induced band
representations of space groups, the full electron state symmetries and the selection rules for
optical transitions in the (GaAs)m(AlAs)n superlattices (SL's) are studied.
The (GaAs)m(AlAs)n [hkl] SL's are a new class of artificially grown crystals whose
structure (i. e. a space group G and an arrangement of atoms over the Wyckoff positions in a
primitive cell) depends on the growth direction [hkl] and numbers of monolayers (m, n) of
constituent materials.
For each direction of growth, these SL's constitute several single crystal families specified
by different space groups Gl' G2' ... Gr By definition, within each family, the crystals have the
same space group Gi but differ from each other by an arrangement of atoms over the Wyckoff
positions. Thus, from the crystallographic point of view, the SL's with different numbers of
monolayers m and n are distinct crystals, even those belonging to the same family.
Such a dependence of the SL crystal structure on the numbers of monoloyers influences on
the phonon and electron states in these crystals. To study the optical properties of SL's one
X III
should know the complete information on their crystal structure.
Knowledge of the optical properties are essential for modeling quantum well laser diode
structures. Many of interactions of quantum wells in lasers derive from the properties of the
density of states function of the two-dimensional electron system. The abrupt edge of the density
of states as a function of energy provides a very high differential gain above transparency leading
to significant reductions in threshold current in appropriately designed devices compared with their
bulk counterparts. In all quantum well lasers the threshold current follows the intrinsic linear
dependence over a low temperature region but as the temperature is increased an approximately
exponential increase in threshold with temperature is superimposed on the linear behavior and this
becomes dominant at sufficiently high temperature. The additional current above the intrinsic
linear component is often referred as the " excess current". Experiments have shown that this
current is chiefly due to non-radiative recombination via deep states in the AlGaAs barrier material
forming the core of the waveguide which contains a higher density of deep states than the GaAs
material comprising the well. Because the carrier density in the barrier increases exponentially
with temperature compared with that in the well, this excess current component has an
exponential temperature dependence.
For visible emitting lasers it is often not sufficient to consider the active region of the
quantum well in isolation from the rest of the device structure. Realistic estimate of the threshold
current, particularly its temperature dependence should include current paths in other parts of the
device structure.
Examine of possible current paths and different assumptions on the physical parameters
leads to the conclusion that the best approach to modeling the current through a laser is a self
consistent simulation of the current flow and potential by numerical solution of the current
continuity equations and Poisson's equation throughout the complete structure, together with the
solution of Schrodinger's equation for a non-square well. Such simulation for 670 urn GaInP
XIV
lasers are presented in detail in this volume. The results give a good description of the temperature
dependence of threshold current and provide tutorial illustrations of the inadequacies of the simple
flat - band model.
An other important feature for the systems based on quantum structure devices are the
Microcavity Semiconductor Lasers. In the chapter on Microcavity Semiconductor Lasers the
theory and recent experimental developments in such lasers and their implications are reviewed.
Particular attention is paid to microdisk lasers which support whispering gallery modes.
InGaAsP/1nP microdisks have recently been pumped optically, resulting in the fist achievement
of ew room temperature lasing in these devices.
The future viability of optoelectronics as a mainstream technology in communications,
computing, data storage and consumer products is contingent on developing efficient, flexible and
controllable photonic emitters, detectors, filters, amplifiers, memory elements and logic devices.
It is intriguing and exiting to consider utilizing the quantum nature of light itself in designing am studing photonic devices of all types. A critical part of this effort is the study of wavelength scale
structures for control and selection of photon modes; structures such as microcavities and the
closely related photonic bandgap materials.
A microcavity laser may be defined operationally as one whose cavity length is comparable
to the emission wavelength, in at least one dimension. A simple example is the planar
microcavity laser whose thin (::::1..) active region is bounded by two parallel, highly reflecting
mirrors. A related structure is the vertical cavity surface - emitting laser (VeSEL) in which a
planar microcavity is modified (by implantation, oxidation, etching or optical pumping) so that
the gain is of limited spatial extent: the cavity is only a few wavelengths long but much larger in
lateral extent.
From a physical point of view, a microcavity may be considered as an atom or atom-like
xv
emitter inside a cavity. In a true microscopic system the dimensions are comparable to the size of
the atom and are thus much smaller than the (optical) wavelength. In a macroscopic system the
dimensions are much greater than the wavelength. A microcavity is therefore a mesoscopic
system, in that its scale is intermediate between those of microscopic and macroscopic objects.
Because of this scaling, it is often possible to adopt a semi-classical point of view, in which the
active atom or atom-like species (in this case the coupled system consisting of an electron in the
conduction band of the semiconductor and the corresponding hole in the valence band) is treated
quantum mechanically and the electromagnetic field is considered classically. From an engineering
or applied - physics perspectives, a microcavity may be considered as a filter or distributor of the
radiation from the aton:..
In the chapter on microcavity lasers the discussion is based on the microdisk laser, in
which light undergoes total internal reflection along the perimeter of an isolated circular disk,
where two-dimensional mode confinement is provided via so-called « whispering gallery modes ».
After a section which outlines some theoretical and fundamental considerations,
particularly regarding the predicted effects of l-D and 2-D microcavities on the density of photon
modes. The fabrication of typical microdisk lasers, recent optical pumping experiments and the
first demonstration of CW room temperature lasing semiconductor microdisk laser are described
and discussed.
MQW Optoelectronic Devices and Systems
Optoelectronic devices are first discussed in a chapter on Exciton Absorption Saturation
and Carrier Transport in quantum Well Semiconductors. Optical nonlinearities associated with
excitonic absorption features in multiple quantum well (MQW) semiconductors offer a number of
useful functions for optoelectronics devices. These include laser mode-locking elements, saturable
elements for controlling the propagation of optical solutions in fibre transmission systems, all-
XV}
optical directional coupler switches and self-electro-optic devices for communications, signal
processing and computing. The operation and optimization of these devices rely on an
understanding of the mechanisms which contribute to absorption saturation and the motion of
optically generated electrons and holes in directions both parallel and perpendicular to the quantum
wells. The chapter on Exciton Absorption Saturation and Carrier Transport in quantum Well
Semiconductors reviews measurements of exiton absorption saturation mechanism and transport
processes (in-well and cross-well) relevant to new optoelectronic electro-optic and nonlinear
optical devices.
Resonant nonlinear and electro-optic interactions are particularly large in quantum wells at
room temperature because of prominent excitonic features in their absorption spectra close to the
band gap energy. Absorption coefficients at the peak of the exciton absorption can be in excess of
104 em -1 providing very efficient absorption in samples only a few microns thick. Optical
excitation of excitons and free carriers can bleach these absorption features by a number of
mechanisms including phase space filling, Coulomb screening and lifetime broadening. Pump
probe measurements using ultrashort pulses of laser light with different linear and circular
polarizations can be used to identify the relative magnitudes of the various contributions.
After creation of the electron and hole pairs, a dynamical situation is produces whereby the
bleaching will relax because of the motion and recombination processes for the free carriers in the
sample. Drift and diffusion properties normally determine the manner in which semiconductor
devices operate but many additional processes in MQW structures have to be considered if we
wish to assess the ultimate performance limits of low dimensional devices. These processes
include thermionic emission from, tunneling through, and trapping into the wells. The ability to
control the motion of electrons and holes by designing the structures to make use of these
processes gives opportunities for engineering devices with new and unique properties. Pump
probe and transient grating techniques can be used to monitor the motion and dynamics of the
carriers on ultrashort time scales using excitonic saturation nonlinearities as the probe.
XVll
Soliton-Based Switching, Gating and Transmission Systems
A large chapter in this volume is devoted to the soliton - based logic gates and soliton
transmission systems. This chapter is a glance into the future since solitons can be considered as
candidates as ''information bits" in telecommunication systems behind the year 2000.
The volume contains also a certain number of short original contributions showing the
present status of the art in quantum systems.
M. BALKANSKI
N. ANDREEV
Acknowledgments
The NATO Advanced Study Institute on "Advanced Electronic Technologies and Systems
based on Low-Dimensional Quantum Devices", held in Sozopol, Bulgaria, September 18-28,
1996, was made possible by an award from the Assistant Secretary General for Scientific and
Environmental Mfairs. We are particularly grateful to Dr. J.A. Rausell-Colom, Program Director
for Priority Area and High technology, for his constant interest and helpful guidance during the
preparation of the AS!.
Of great value for the present success of this school and the future development of a Center
for Scientific Culture in Bulgaria is the personal involvement of Dip. Eng. Peter Kimenov,
General Manager of Administration Department of Bulbank and that of Dichko Fotev,
Administrator of the Sozopol Pochivna Basa of Bulbank.
We owe special thank to the rector of Sofia University, Professor Ivan Lalov, who not
only supported very generously the whole process of the organization of the school, but also
came to Sozopol to attest with his presence his personal interest in the development of scientific
culture in Bulgaria. Many colleagues from Sofia University and from the Technical University
have generously helped the organization of the school and we are grateful for their involvement.
We also wish to thanks Dr. Stoyan Tanev for giving so much of his energy mxl
enthusiasm to the enterprise. Lucy Nedialkova has also generously helped the preparation of the
book based on the lectures of the School.
xix