Quantum Mechanics for Scientists and Engineers

Couverture
Cambridge University Press, 21 avr. 2008 - 574 pages
If you need a book that relates the core principles of quantum mechanics to modern applications in engineering, physics, and nanotechnology, this is it. Students will appreciate the book's applied emphasis, which illustrates theoretical concepts with examples of nanostructured materials, optics, and semiconductor devices. The many worked examples and more than 160 homework problems help students to problem solve and to practise applications of theory. Without assuming a prior knowledge of high-level physics or classical mechanics, the text introduces Schrödinger's equation, operators, and approximation methods. Systems, including the hydrogen atom and crystalline materials, are analyzed in detail. More advanced subjects, such as density matrices, quantum optics, and quantum information, are also covered. Practical applications and algorithms for the computational analysis of simple structures make this an ideal introduction to quantum mechanics for students of engineering, physics, nanotechnology, and other disciplines. Additional resources available from www.cambridge.org/9780521897839.

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Pages sélectionnées

Table des matières

hapter
1
Waves and quantum mechanics Schrödingers equation
8
multiplying by a constant
16
7
23
9
29
10
39
12
46
The timedependent Schrödinger equation
54
Spin
297
Identical particles
311
The density matrix
335
Harmonic oscillators and photons
354
Quantum mechanical states of an electromagnetic field mode
370
Vibrational modes
378
15
380
16
392

5
60
7
66
10
77
13
85
Functions and operators
93
Operators and quantum mechanics
129
Approximation methods in quantum mechanics
154
Timedependent perturbation theory
182
Quantum mechanics in crystalline materials
207
Chapter 9
242
1
257
Chapter 11
277
Interaction of different kinds of particles
406
Quantum information
424
Interpretation of quantum mechanics
441
Appendix A Background mathematics
457
Appendix B Background physics
491
Vector calculus
499
Maxwells equations and electromagnetism
509
Appendix E Perturbing Hamiltonian for optical absorption
519
Appendix F Early history of quantum mechanics
523
Memorization list
539
335
545
Droits d'auteur

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Fréquemment cités

Page 81 - V = , , (2.45) dy dz where i, j and k are unit vectors in the x, y and z directions respectively.
Page 233 - The determinant in (3) is of dimensions 9N x 9N, where N is the number of unit cells in the crystal, and...
Page 227 - JM Luttinger and W. Kohn. Motion of electrons and holes in perturbed periodic fields.
Page 427 - CH Bennett, F. Bessette, G. Brassard, L. Salvail, and J. Smolin, Experimental quantum cryptography, Journal of Cryptology, vol.
Page 450 - The fact that an adequate philosophical presentation has been so long delayed is no doubt caused by the fact that Niels Bohr brainwashed a whole generation of theorists into thinking that the job was done fifty years ago (Gell-Mann, 1979).
Page 468 - A differential equation is an equation that involves one or more derivatives, or differentials. Differential equations are classified by (a) type: ordinary or partial, (b) order: the order of the highest-order derivative that occurs in the equation, (c) degree: the exponent of the highest power of the highest-order derivative, after the equation has been cleared of fractions...
Page 427 - Quantum key distribution over a 48 km optical fiber network,
Page 460 - Since we are plotting log-magnitude, we can use the fact that the log of a product is the sum of the logs.
Page i - He is a fellow of the Royal Society, the Royal Society of Edinburgh...
Page 515 - ... panel and the flange on the box (the foil was not conductively connected to the fibers of the composite) . Tests with Frame Fixtures In all tests using the frame fixtures, identical 10 inch by 15 inch panels were mounted on both faces of the frame. The panels and fixture were then illuminated by a plane wave linearly polarized in the x direction and propagating in the y direction (see Figure 4). Electric field shielding was measured with a rod antenna, while magnetic field shielding was measured...

À propos de l'auteur (2008)

David A. B. Miller received the B.Sc. degree from St Andrews University, and, in 1979, the Ph.D. degree from Heriot-Watt University, both in Physics. He was with Bell Laboratories from 1981 to 1996, as a department head from 1987, latterly of the Advanced Photonics Research Department. He is currently the W. M. Keck Professor of Electrical Engineering, the Director of the Solid State and Photonics Laboratory, and a Co-Director of the Stanford Photonics Research Center at Stanford University, Stanford, California, USA. His research interests include physics and devices in nanophotonics, nanometallics, and quantum-well optoelectronics, and fundamentals and applications of optics in information sensing, switching, and processing. He has published more than 200 scientific papers, holds 62 patents, is a Fellow of OSA, IEEE, APS, and the Royal Societies of Edinburgh and London, holds honorary degrees from the Vrije Universiteit Brussel and Heriot-Watt University, and has received numerous awards.

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