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1 wave mechanics applied to semiconductor heterostructures GERALD BASTARD les editions de physique Avenue du Hoggar, Zone Industrielle de Courtaboeuf, B.P. 112, Les Ulis Cedex, France
2 Contents PREFACE page III CHAPTER I : IDEALIZED QUANTUM WELLS AND SUPER- LATTICES. A SUMMARY page 1 I. Single quantum wells 1 II. Density of states 11 III. Tunnel coupling between wells: the Symmetrie double Square well 14 IV. Superlattices 18 IV. 1. Superlattice dispersion relations 18 IV.2. Symmetry properties of the eigenfunetions 23 IV.3. Superlattice density of states 24 APPENDIX A : Symmetrie double square well. Time-dependent aspect. 27 APPENDIX B : Dispersion relations of superlattices witft arbitrary Potential profiles 28 CHAPTER II : BAND STRUCTURE OF BULK III-V COMPOUNDS page 31 I. Crystalline properties 31 II. Electronic properties 32 III. Electronic dispersion relations in the vicinity of the zone centre : k.p analysis and Kane model 35 III. 1. k.p analysis and effective masses Effective mass tensor. Electrons and holes Beyond the quadratic dispersion relations : the Kane model.. 41 a) Dispersions relations of the Kane model 41 b) Band edge effective masses 45 c) Band non parabolicity 46 d) Inclusion of higher bands 46 e) Accuracy of the Kane model 47 IV. Conclusions 49 APPENDIX A : Inclusion of remote bands effects 50 APPENDIX B : Motion of Kane electrons in slowly varying perturbing fields 54
3 VI Wave mechanics applied to semiconductor heterostructures CHAPTER III : ENVELOPE FUNCTION DESCRIPTION OF HETE- ROSTRUCTURE ELECTRONIC STATES page 63 I. Introduction 63 II. The envelope function model Preliminaries The envelope function framework The Ben Daniel-Duke model The Ben Daniel-Duke quantum wells (m A m B > 0) Interface states of Ben Daniel-Duke quantum wells (w A m B < 0 ; * ± =0) Quantum wells and superlattices with hosts which display Kane-like bands Simplified calculations of superlattices and quantum wells states k ± = Miscelleanous limiting cases Evanescent propagation in one kind of layer. Quantum well bound states Tight-binding expansion of the superlattice states Propagating states in both kinds of layers Heavy hole superlattice states Specific examples Labelling and counting superlattice states 100 III. In-plane dispersions in semiconductor heterostructures 101 APPENDIX A : Boundary conditions and stationary states 112 APPENDIX B : Coupling between light and heavy particle states due to inversion asymmetry Splitting in bulk materials. Qualitative aspects 113 CHAPTER IV : COULOMBIC BOUND STATES AND INTERFACE DEFECTS IN HETEROSTRUCTURES page 119 Coulombic bound states I. Qualitative aspects Bulk hydrogenic impurities Impurities in heterostructures 120 II. Approximate Solutions of the hydrogenic impurity problem 121 II. 1. Formulation of the problem Results for the ground impurity State attached to the ground subband Excited subbands. Continuum Excited impurity levels attached to the ground subband Acceptor levels in a quantum well 128
4 Contents VII III. Excitons 128 III. 1. Excitons in idealized bulk materials Excitons in idealized quantum well structures Excitons in actual quantum well structures 139 Interface defects I. Graded interfaces 142 II. Quantum well interface defects 143 III. Superlattice defect states 149 APPENDIX : Energy levels in a quantum well with narrow graded interfaces 151 CHAPTER V : ENERGY LEVELS IN MODULATION-DOPED HETEROSTRUCTURES page 155 I. The modulation doping of heterojunctions. Qualitative aspects The unperturbed heterojunction (flat band case) Single heterojunction containing diluted Coulombic impurities Actual heterostructures 160 II. Seif consistent calculations of energy levels and Charge transfer in Single heterojunctions 161 II. 1. Energy level calculations Charge transfer in Single heterojunctions 172 III. Energy levels in modulation-doped quantum wells 180 APPENDIX A : The algebra of the modified Fang Howard wavefunction 186 APPENDIX B : Heterojunction energy levels : qualitative aspects 188 CHAPTER VI : ELECTRICAL CONDUCTIVITY OF QUASI BI- DIMENSIONAL ELECTRON GASES page 193 I. Static conductivity of a quasi bi-dimensional electron gas Electrical conductivity in the electric quantum limit Intersubband scattering Screening in a quasi bi-dimensional electron gas. Application to Coulombic impurities Discussion of the dielectric function 207 II. Evaluation of some scattering mechanisms 212 II. 1. Mobility limited by Coulombic scattering 212 H.2. AUoy scattering Interface roughness scattering 223 III. Vertical transport 225 IV. Resonant tunnelling 228 APPENDIX : Dimensional dependence of the Screening effects 233
5 VIII Ware mechanics applied to semiconductor heterostructures CHAPTER VII : OPTICAL PROPERTIES OF QUASI BI-DIMEN- SIONAL SYSTEMS page 237 I. Absorption (one-electron approximation) Intraband transitions Interband transitions Polarization selection rules Selection rules on the envelope function quantum numbers : evaluation of < f/f f > Order of magnitude of the absorption coefficient. Comparison between type I and type II Systems Interband optical transitions in superlattices 255 II. Absorption : a simplified description of excitonic effects 258 II. 1. Absorption in the absence of Coulombic interactions. Equivalence with the one-electron model 260 II.2. Absorption in the presence of electron-electron interactions III. Photoluminescence of quasi bi-dimensional Systems Introduction Quantum well luminescence (steady State) Band to band emission Excitonic recombination Extrinsic photoluminescence 295 CHAPTER VIII : EFFECT OF STATIC EXTERNAL ELECTRIC AND MAGNETIC FIELDS ON THE ENERGY LEVELS OF QUASI BI-DIMENSIONAL ELEC TRON GASES page 303 I. The Stark effects Transverse Stark effect in a quantum well (F//x) Longitudinal Stark effect in a quantum well (F//z) 308 II. Landau quantization of a quasi bi-dimensional electron gas Energy levels Magnetic field dependent density of states Magnetoconductivity of a quasi bi-dimensional electron gas Macroscopic derivation Microscopic discussion Cyclotron resonance 339 APPENDIX A : Motion of three-dimensional electrons in crossed electric and magnetic fields 345 AI. The Drude model 346 All. Quantum motion of bulk electrons in a magnetic field 348 APPENDIX B : Microscopic evaluation of the magnetoconductivity tensor 351
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