## Solid state physics |

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Page 40

One speaker is moved back by a half

interfere. that when one wave is up, the other is down, and vice versa. The

algebraic sum of these two waves is zero. The resultant wave has zero amplitude

. The two ...

One speaker is moved back by a half

**wavelength**. These waves destructivelyinterfere. that when one wave is up, the other is down, and vice versa. The

algebraic sum of these two waves is zero. The resultant wave has zero amplitude

. The two ...

Page 68

(3-12) Comparing with Eq. (3-11), we see that this wave has a velocity, v = wma/2

, (3-13) which is independent of

line in Fig. 3-6. Note that the dashed line is a good approximation to the actual ...

(3-12) Comparing with Eq. (3-11), we see that this wave has a velocity, v = wma/2

, (3-13) which is independent of

**wavelength**. Eq. (3-12) is shown as a dashedline in Fig. 3-6. Note that the dashed line is a good approximation to the actual ...

Page 111

Find the difference in

one of the TA peaks of Fig. 5-6. Answer: 0.7 A. 5-5 Wave-like Properties of

Particles We have seen that waves sometimes behave like particles with

momentum p ...

Find the difference in

**wavelength**of the photons in the central peak and those inone of the TA peaks of Fig. 5-6. Answer: 0.7 A. 5-5 Wave-like Properties of

Particles We have seen that waves sometimes behave like particles with

momentum p ...

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### Contents

XRay Diffraction | 37 |

Lattice Vibrations | 61 |

Classical Model of Metals | 89 |

Copyright | |

12 other sections not shown

### Common terms and phrases

Answer Appendix basis vectors bcc lattice bond Bragg angle Bragg's Law Bravais lattice Brillouin zone called Chapter collisions conduction electrons Consider conventional unit cell Cooper pairs depletion layer diode direction dispersion curve displacement distance doped effective mass elec electric current electric field electrons and holes emitter energy band equal example Fermi energy Fermi level Fermi surface force forward biased free electron free particle frequency given by Eq inside integers ions k-space laser lattice parameter lattice points lattice vector lattice wave magnetic field n-type semiconductor NaCl negative neutrons number of electrons obtain occupied one-dimensional oscillate p-n junction photon positively charged potential energy primitive unit cell Problem rays reciprocal lattice reverse biased sc lattice scattered Schroedinger's equation shown in Fig sodium metal solid structure superconductor temperature tion transistor trons unit cell unoccupied values velocity voltage wave function wave number wave vector wavelength Wigner-Seitz cell wire x-ray diffraction zero