## Introduction to Solid State Physics |

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Page 249

The level which divides the filled and vacant levels is known as the

absolute zero and is denoted by E.F(0). There is considerable interest in knowing

the value of the

The level which divides the filled and vacant levels is known as the

**Fermi**level atabsolute zero and is denoted by E.F(0). There is considerable interest in knowing

the value of the

**Fermi**level as a function of the electron concentration N. The ...Page 251

On heating from absolute zero every electron does not gain an energy -kT as

happens classically, but only those electrons already within an energy range of

the order of kT of the

an ...

On heating from absolute zero every electron does not gain an energy -kT as

happens classically, but only those electrons already within an energy range of

the order of kT of the

**Fermi**level can be excited thermally; these electrons gainan ...

Page 612

F' centers, 495 Face-centered cubic lattice, 28 Brillouin zone, 314

distribution law, 251, 254

for metals, 250

F' centers, 495 Face-centered cubic lattice, 28 Brillouin zone, 314

**Fermi**–Diracdistribution law, 251, 254

**Fermi**energy, 249, 254**Fermi**level, 249, 254, 590 tablefor metals, 250

**Fermi**temperature, 249 Ferrimagnetism, definition, 445 Ferrites, ...### What people are saying - Write a review

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absorption acceptors alkali alloys approximately atoms axis barium titanate boundary Bragg Brillouin zone calculated chapter charge conduction band conduction electrons crystal structure cube cubic Curie point Debye density dielectric constant diffraction diffusion dipole direction discussion dislocation distribution domain effective mass elastic electric field energy equation equilibrium exciton experimental F centers factor Fermi ferroelectric ferromagnetic free electron frequency germanium given heat capacity hexagonal holes impurity interaction ionization ions lattice constant lattice point low temperatures magnetic field magnetic moment metals molecules motion nearest neighbor normal observed p-n junction paramagnetic particles phonons Phys physics plane polarizability polarization positive potential Proc region resonance result room temperature rotation semiconductor Shockley shown in Fig sodium chloride solid solution space group specimen spin superconducting surface susceptibility symmetry Table theory thermal tion transition unit volume vacancies valence band values vector velocity wave functions wavelength zero