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Title:
Non-Hermitian quantum mechanics
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Publication Information:
Cambridge ; New York : Cambridge University Press, 2011
Physical Description:
xiii, 394 p. : ill. ; 26 cm.
ISBN:
9780521889728

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30000010321523 QC174.17.M35 M65 2011 Open Access Book Book
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Summary

Summary

Non-Hermitian quantum mechanics (NHQM) is an important alternative to the standard (Hermitian) formalism of quantum mechanics, enabling the solution of otherwise difficult problems. The first book to present this theory, it is useful to advanced graduate students and researchers in physics, chemistry and engineering. NHQM provides powerful numerical and analytical tools for the study of resonance phenomena - perhaps one of the most striking events in nature. It is especially useful for problems whose solutions cause extreme difficulties within the structure of a conventional Hermitian framework. NHQM has applications in a variety of fields, including optics, where the refractive index is complex; quantum field theory, where the parity-time (PT) symmetry properties of the Hamiltonian are investigated; and atomic and molecular physics and electrical engineering, where complex potentials are introduced to simplify numerical calculations.


Author Notes

Nimrod Moiseyev is Bertha Hartz Axel Professor of Chemistry and Physics and a member of the joint Minerva Centre for Nonlinear Physics of Complex Systems at the Technion-Israel Institute of Technology. He has won numerous awards for his work, including the Humboldt Prize, the Marie Curie Prize, and the Landau Prize for major contribution to the development of the non-Hermitian theory of quantum mechanics.


Table of Contents

Prefacep. xi
1 Different formulations of quantum mechanicsp. 1
1.1 Hermitian operators: a brief reviewp. 3
1.2 Non-Hermitian potentials which support a continuous spectrump. 4
1.3 Complex local potentialsp. 10
1.4 Physical interpretation of complex expectation valuesp. 11
1.5 Concluding remarksp. 12
1.6 Solutions to the exercisesp. 13
1.7 Further readingp. 19
2 Resonance phenomena in naturep. 21
2.1 Shape-type resonancesp. 21
2.2 Feshbach-type resonancesp. 25
2.3 Concluding remarksp. 31
2.4 Solutions to the exercisesp. 33
2.5 Further readingp. 39
3 Resonances from Hermitian quantum-mechanical calculationsp. 41
3.1 Resonances as metastable statesp. 41
3.2 The poles of the S-matrixp. 45
3.3 Resonances from the spectra of density of statesp. 46
3.4 Resonances from the asymptotes of continuum eigenfunctionsp. 50
3.5 Resonances from the phase shiftsp. 54
3.6 The scattering lengthp. 57
3.7 Resonances from stabilization calculationsp. 60
3.8 Decay of resonance statesp. 64
3.9 Real and complex poles of the scattering matrix from wavepacket propagation calculationsp. 70
3.10 Concluding remarksp. 71
3.11 Solutions to the exercisesp. 72
3.12 Further readingp. 82
4 Resonances from non-Hermitian quantum mechanical calculationsp. 84
4.1 Resonances for a time-independent Hamiltonianp. 86
4.2 Transitions of bound states to anti-bound and resonance statesp. 91
4.3 Bound, virtual and resonance states for a 1D potentialp. 95
4.4 The mechanism of transition from a bound state to a resonance statep. 97
4.5 Concluding remarks on the physical and non-physical poles of the S-matrixp. 101
4.6 Resonances for a time-dependent Hamiltonianp. 102
4.7 Conservation of number of particlesp. 104
4.8 Solutions to the exercisesp. 106
4.9 Further readingp. 115
5 Square integrable resonance wavefunctionsp. 116
5.1 The Zel'dovich transformationp. 118
5.2 The complex scaling transformationp. 120
5.3 The exterior scaling transformationp. 127
5.4 The smooth exterior scaling transformationp. 129
5.5 Dilation of the Hamiltonian matrix elements into the complex planep. 133
5.6 Square integrability of field induced resonancesp. 136
5.7 Partial widths from the tails of the wavefunctionsp. 142
5.8 Concluding remarksp. 147
5.9 Solutions to the exercisesp. 149
5.10 Further readingp. 169
6 Bi-orthogonal product (c-product)p. 174
6.1 The c-productp. 174
6.2 Completeness of the spectrump. 183
6.3 Advantages of calculating survival probabilities by c-productp. 186
6.4 The c-product for non-Hermitian time-periodic Hamiltoniansp. 188
6.5 The F-product for time propagated wavepacketsp. 190
6.6 The F-product and the conservation of the number of particlesp. 195
6.7 Concluding remarksp. 196
6.8 Solutions to the exercisesp. 197
6.9 Further readingp. 210
7 The properties of the non-Hermitian Hamiltonianp. 211
7.1 The turn-over rulep. 211
7.2 The complex analog of the variational principlep. 213
7.3 The complex analogs of the virial and hypervirial theoremp. 225
7 4 The complex analog of the Hellmann-Feynman theoremp. 226
7.5 Cusps and 0-trajectoriesp. 227
7.6 Upper and lower bounds of the resonance positions and widthsp. 230
7.7 Perturbation theory for non-Hermitian Hamiltoniansp. 235
7.8 Concluding remarksp. 237
7.9 Solutions to the exercisep. 238
7.10 Further readingp. 247
8 Non-Hermitian scattering theoryp. 250
8.1 Full collision processes for time-independent Systemsp. 254
8.2 Half collision processes for time-independent Systemsp. 266
8.3 Time-independent scattering theory for time-dependent Systemsp. 275
8.4 Solutions to the exercisesp. 309
8.5 Further readingp. 318
9 The self-orthogonality phenomenonp. 323
9.1 The phenomenon of self-orthogonalityp. 324
9.2 On self-orthogonality and the closure relationsp. 334
9.3 Calculations of the radius of convergence of perturbational expansion of the eigenvalues in V 0p. 342
9.4 The effect of self-orthogonality on c-expectation valuesp. 343
9.5 Zero resonance contribution to the cross sectionp. 350
9.6 Geometric phases (Berry phases)p. 351
9.7 Concluding remarksp. 358
9.8 Solutions to the exercisesp. 359
9.9 Further readingp. 373
10 The point where QM branches into two formalismsp. 375
10.1 Feshbach resonancesp. 375
10.2 The point where QM branches into two formalismsp. 379
10.3 Concluding remarksp. 387
10.4 Solutions to the exercisesp. 387
10.5 Further readingp. 391
Indexp. 393