## Solid state physics |

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Page 144

This requires that Eq. (7-20) be equal to Eq. (7-21): Wx2Px{l - P2) = W21P2{1 -

P1). (7-22) Combining this with Eq. (7-19) and rearranging the terms, we

exp(E1/fcBr) = exp(E2/kBT). (7-23) 1 - f\ 1 - r2 Since states 1 and 2 were chosen ...

This requires that Eq. (7-20) be equal to Eq. (7-21): Wx2Px{l - P2) = W21P2{1 -

P1). (7-22) Combining this with Eq. (7-19) and rearranging the terms, we

**obtain**exp(E1/fcBr) = exp(E2/kBT). (7-23) 1 - f\ 1 - r2 Since states 1 and 2 were chosen ...

Page 199

When we do the integral in Eq. (10-11), we

<M3) Since the number of holes in the VB is equal to the number of electrons in

the CB, we must have n = p. Setting Eqs. (10-10) and (10-13) equal to each ...

When we do the integral in Eq. (10-11), we

**obtain**fm;kBT\3/2 ( EF \ , '-'{-tar) exp (1<M3) Since the number of holes in the VB is equal to the number of electrons in

the CB, we must have n = p. Setting Eqs. (10-10) and (10-13) equal to each ...

Page 226

Since the total charge at the junction is zero, the electric field must be zero at an

infinite distance away (either in the +x or -x direction). Thus we can

by integrating Eq. (11-10) from -co to x: f p dx. (11-11) Using the function shown

in ...

Since the total charge at the junction is zero, the electric field must be zero at an

infinite distance away (either in the +x or -x direction). Thus we can

**obtain**<£(x)by integrating Eq. (11-10) from -co to x: f p dx. (11-11) Using the function shown

in ...

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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