My Account Log in

1 option

The k-p method : electronic properties of semiconductors / Lok C. Lew Yan Voon, Morten Willatzen.

Van Pelt Library TK7871.85 L46 2009
Loading location information...

Available This item is available for access.

Log in to request item
Format:
Book
Author/Creator:
Lew Yan Voon, Lok C.
Contributor:
Willatzen, Morten.
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

The Penn Libraries is committed to describing library materials using current, accurate, and responsible language. If you discover outdated or inaccurate language, please fill out this feedback form to report it and suggest alternative language.

Find

Home Release notes

My Account

Shelf Request an item Bookmarks Fines and fees Settings

Guides

Using the Find catalog Using Articles+ Using your account