## Solid state physics |

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Page 145

5>£: (7-28» This means that the probability that a state below the

occupied is equal to 1, and the probability that a state above the

occupied is equal to 0. All states below Ep are occupied and all states above Ep

are ...

5>£: (7-28» This means that the probability that a state below the

**Fermi level**isoccupied is equal to 1, and the probability that a state above the

**Fermi level**isoccupied is equal to 0. All states below Ep are occupied and all states above Ep

are ...

Page 223

Ei CB gap rf\ rf\ rf\ /T\ rf\ /T\ /T\ /T\ /T\ 1JI VB eeeeeeeee

side Fig. 11-7.

?). (11-6) In Fig. 11-7 is the energy diagram of the junction with the

Ei CB gap rf\ rf\ rf\ /T\ rf\ /T\ /T\ /T\ /T\ 1JI VB eeeeeeeee

**Fermi level**-m- X p-side n-side Fig. 11-7.

**Fermi level**across a p-n junction. Thus, <j> = {kBT/e) ln(JVdJVa/n?). (11-6) In Fig. 11-7 is the energy diagram of the junction with the

**Fermi level**...Page 236

What happens to the

The electrons and holes are not in a state of equilibrium (they are flowing). Thus,

the

...

What happens to the

**Fermi level**when the p-n junction is conducting a current?The electrons and holes are not in a state of equilibrium (they are flowing). Thus,

the

**Fermi level**is not the same on both sides of the junction. When the junction is...

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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