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The k-p method : electronic properties of semiconductors / Lok C. Lew Yan Voon, Morten Willatzen.
Van Pelt Library TK7871.85 L46 2009
Available
- Format:
- Book
- Author/Creator:
- Lew Yan Voon, Lok C.
- Language:
- English
- Subjects (All):
- Semiconductors.
- Hamiltonian systems.
- Physical Description:
- xxi, 445 pages : illustrations ; 25 cm
- Place of Publication:
- Dordrecht ; New York : Springer, [2009]
- Summary:
- This book presents a detailed exposition of the formalism and application of k.p theory for both bulk and nanostructured semiconductors. For bulk crystals, this is the first time all the major techniques for deriving the most popular Hamiltonians have been provided in one place. For nanostructures, this is the first time the Burt-Foreman theory has been made accessible. Thus, the reader will gain a clear understanding of the k.p method, will have an explicit listing of the various Hamiltonians in a consistent notation for their use, and a set of representative results. In addition, the reader can derive an excellent understanding of the electronic structure of semiconductors.
- Contents:
- 1 Introduction 1
- 1.1 What Is k. p Theory? 1
- 1.2 Electronic Properties of Semiconductors 1
- 1.3 Other Books 3
- Part I Homogeneous Crystals
- 2 One-Band Model 7
- 2.1 Overview 7
- 2.2 k. p Equation 7
- 2.3 Perturbation Theory 9
- 2.4 Canonical Transformation 9
- 2.5 Effective Masses 12
- 2.5.1 Electron 12
- 2.5.2 Light Hole 13
- 2.5.3 Heavy Hole 14
- 2.6 Nonparabolicity 14
- 2.7 Summary 15
- 3 Perturbation Theory - Valence Band 17
- 3.1 Overview 17
- 3.2 Dresselhaus-Kip-Kittel Model 17
- 3.2.1 Hamiltonian 17
- 3.2.2 Eigenvalues 21
- 3.2.3 L, M, N Parameters 22
- 3.2.4 Properties 30
- 3.3 Six-Band Model for Diamond 32
- 3.3.1 Hamiltonian 32
- 3.3.2 DKK Solution 40
- 3.3.3 Kane Solution 43
- 3.4 Wurtzite 45
- 3.4.1 Overview 45
- 3.4.2 Basis States 46
- 3.4.3 Chuang-Chang Hamiltonian 46
- 3.4.4 Gutsche-Jahne Hamiltonian 52
- 3.5 Summary 54
- 4 Perturbation Theory - Kane Models 55
- 4.1 Overview 55
- 4.2 First-Order Models 55
- 4.2.1 Four-Band Model 56
- 4.2.2 Eight-Band Model 57
- 4.3 Second-Order Kane Model 61
- 4.3.1 Löwdin Perturbation 61
- 4.3.2 Four-Band Model 62
- 4.4 Full-Zone k. p Model 64
- 4.4.1 15-Band Model 64
- 4.4.2 Other Models 69
- 4.5 Wurtzite 69
- 4.5.1 Four-Band: Andrew-O'Reilly 70
- 4.5.2 Eight-Band: Chuang-Chang 71
- 4.5.3 Eight-Band: Gutsche-Jahne 71
- 4.6 Summary 77
- 5 Method of Invariants 79
- 5.1 Overview 79
- 5.2 DKK Hamiltonian - Hybrid Method 79
- 5.3 Formalism 84
- 5.3.1 Introduction 84
- 5.3.2 Spatial Symmetries 84
- 5.3.3 Spinor Representation 88
- 5.4 Valence Band of Diamond 88
- 5.4.1 No Spin 89
- 5.4.2 Magnetic Field 90
- 5.4.3 Spin-Orbit Interaction 93
- 5.5 Six-Band Model for Diamond 114
- 5.5.1 Spin-Orbit Interaction 115
- 5.5.2 k-Dependent Part 115
- 5.6 Four-Band Model for Zincblende 116
- 5.7 Eight-Band Model for Zincblende 117
- 5.7.1 Weiler Hamiltonian 117
- 5.8 14-Band Model for Zincblende 120
- 5.8.1 Symmetrized Matrices 121
- 5.8.2 Invariant Hamiltonian 123
- 5.8.3 T Basis Matrices 125
- 5.8.4 Parameters 128
- 5.9 Wurtzite 132
- 5.9.1 Six-Band Model 132
- 5.9.2 Quasi-Cubic Approximation 136
- 5.9.3 Eight-Band Model 137
- 5.10 Method of Invariants Revisited 140
- 5.10.1 Zincblende 140
- 5.10.2 Wurtzite 146
- 5.11 Summary 151
- 6 Spin Splitting 153
- 6.1 Overview 153
- 6.2 Dresselhaus Effect in Zincblende 154
- 6.2.1 Conduction State 154
- 6.2.2 Valence States 154
- 6.2.3 Extended Kane Model 156
- 6.2.4 Sign of Spin-Splitting Coefficients 160
- 6.3 Linear Spin Splittings in Wurtzite 161
- 6.3.1 Lower Conduction-Band e States 163
- 6.3.2 A, B, C Valence States 164
- 6.3.3 Linear Spin Splitting 165
- 6.4 Summary 166
- 7 Strain 167
- 7.1 Overview 167
- 7.2 Perurbation Theory 167
- 7.2.1 Strain Hamiltonian 167
- 7.2.2 Löwdin Renormalization 170
- 7.3 Valence Band of Diamond 170
- 7.3.1 DKK Hamiltonian 171
- 7.3.2 Four-Band Bir-Pikus Hamiltonian 171
- 7.3.3 Six-Band Hamiltonian 172
- 7.3.4 Method of Invariants 174
- 7.4 Strained Energies 177
- 7.4.1 Four-Band Model 177
- 7.4.2 Six-Band Model 179
- 7.4.3 Deformation Potentials 179
- 7.5 Eight-Band Model for Zincblende 180
- 7.5.1 Perturbation Theory 181
- 7.5.2 Method of Invariants 182
- 7.6 Wurtzite 183
- 7.6.1 Perturbation Theory 183
- 7.6.2 Method of Invariants 184
- 7.6.3 Examples 186
- 7.7 Summary 186
- Part II Nonperiodic Problem
- 8 Shallow Impurity States 189
- 8.1 Overview 189
- 8.2 Kittel-Mitchell Theory 190
- 8.2.1 Exact Theory 191
- 8.2.2 Wannier Equation 193
- 8.2.3 Donor States 194
- 8.2.4 Acceptor States 197
- 8.3 Luttinger-Kohn Theory 198
- 8.3.1 Simple Bands 199
- 8.3.2 Degenerate Bands 210
- 8.3.3 Spin-Orbit Coupling 213
- 8.4 Baldereschi-Lipari Model 214
- 8.4.1 Hamiltonian 216
- 8.4.2 Solution 217
- 8.5 Summary 219
- 9 Magnetic Effects 221
- 9.1 Overview 221
- 9.2 Canonical Transformation 222
- 9.2.1 One-Band Model 222
- 9.2.2 Degenerate Bands 230
- 9.2.3 Spin-Orbit Coupling 232
- 9.3 Valence-Band Landau Levels 235
- 9.3.1 Exact Solution 235
- 9.3.2 General Solution 239
- 9.4 Extended Kane Model 240
- 9.5 Land ̌g-Factor 240
- 9.5.1 Zincblende 241
- 9.5.2 Wurtzite 243
- 9.6 Summary 244
- 10 Electric Field 245
- 10.1 Overview 245
- 10.2 One-Band Model of Stark Effect 245
- 10.3 Multiband Stark Problem 246
- 10.3.1 Basis Functions 246
- 10.3.2 Matrix Elements of the Coordinate Operator 248
- 10.3.3 Multiband Hamiltonian 249
- 10.3.4 Explicit Form of Hamiltonian Matrix Contributions 253
- 10.4 Summary 255
- 11 Excitons 257
- 11.1 Overview 257
- 11.2 Excitonic Hamiltonian 258
- 11.3 One-Band Model of Excitons 259
- 11.4 Multiband Theory of Excitons 261
- 11.4.1 Formalism 261
- 11.4.2 Results and Discussions 266
- 11.4.3 Zincblende 267
- 11.5 Magnetoexciton 268
- 11.6 Summary 270
- 12 Heterostructures: Basic Formalism 273
- 12.1 Overview 273
- 12.2 Bastard's Theory 274
- 12.2.1 Envelope-Function Approximation 274
- 12.2.2 Solution 276
- 12.2.3 Example Models 277
- 12.2.4 General Properties 279
- 12.3 One-Band Models 280
- 12.3.1 Derivation 280
- 12.4 Burt-Foreman Theory 282
- 12.4.1 Overview 283
- 12.4.2 Envelope-Function Expansion 283
- 12.4.3 Envelope-Function Equation 287
- 12.4.4 Potential-Energy Term 294
- 12.4.5 Conventional Results 299
- 12.4.6 Boundary Conditions 305
- 12.4.7 Burt-Foreman Hamiltonian 306
- 12.4.8 Beyond Burt-Foreman Theory? 316
- 12.5 Sercel-Vahala Theory 318
- 12.5.1 Overview 318
- 12.5.2 Spherical Representation 319
- 12.5.3 Cylindrical Representation 324
- 12.5.4 Four-Band Hamiltonian in Cylindrical Polar Coordinates 329
- 12.5.5 Wurtzite Structure 336
- 12.6 Arbitrary Nanostructure Orientation 350
- 12.6.1 Overview 350
- 12.6.2 Rotation Matrix 350
- 12.6.3 General Theory 352
- 12.6.4 [11̄0] Quantum Wires 353
- 12.7 Spurious Solutions 360
- 12.8 Summary 361
- 13 Heterostructures: Further Topics 363
- 13.1 Overview 363
- 13.2 Spin Splitting 363
- 13.2.1 Zincblende Superlattices 363
- 13.3 Strain in Heterostructures 367
- 13.3.1 External Stress 367
- 13.3.2 Strained Heterostructures 369
- 13.4 Impurity States 371
- 13.4.1 Donor States 371
- 13.4.2 Acceptor States 372
- 13.5 Excitons 373
- 13.5.1 One-Band Model 373
- 13.5.2 Type-II Excitons 376
- 13.5.3 Multiband Theory of Excitons 377
- 13.6 Magnetic Problem 378
- 13.6.1 One-Band Model 379
- 13.6.2 Multiband Model 382
- 13.7 Static Electric Field 384
- 13.7.1 Transverse Stark Effect 384
- 13.7.2 Longitudinal Stark Effect 386
- 13.7.3 Multiband Theory 388
- 14 Conclusion 391.
- Notes:
- Includes bibliographical references (pages 431-442) and index.
- ISBN:
- 9783540928713
- 3540928715
- OCLC:
- 310401070
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