## Solid state physics |

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Page 47

As an example,

separated by a distance d = 3.0 A. From Eq. (2-10), we find that sin0 = n\/2d, and

thus 0 = 15°, 31°, 51° for n = 1,2,3, respectively. Problem 2-6.

As an example,

**consider**diffraction of x rays (A = 1.542 A) from planes of atomsseparated by a distance d = 3.0 A. From Eq. (2-10), we find that sin0 = n\/2d, and

thus 0 = 15°, 31°, 51° for n = 1,2,3, respectively. Problem 2-6.

**Consider**a set of ...Page 63

Since we will

between atoms by "springs," each with the appropriate spring constant a. As we

saw above, a pair of atoms connected by a spring simply oscillates at some well

defined ...

Since we will

**consider**only small oscillations, we can replace real forcesbetween atoms by "springs," each with the appropriate spring constant a. As we

saw above, a pair of atoms connected by a spring simply oscillates at some well

defined ...

Page 238

Problem 11-13.

junction with 10.0 V, find the width of the depletion layer (er=12 in Si). Answer:

5.30 ^m. 11-9 Capacitance of Junction A p-n junction has capacitance. As we can

see ...

Problem 11-13.

**Consider**the junction in Problem 11-4. If we reverse-bias thisjunction with 10.0 V, find the width of the depletion layer (er=12 in Si). Answer:

5.30 ^m. 11-9 Capacitance of Junction A p-n junction has capacitance. As we can

see ...

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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