## Introduction to Solid State Physics |

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Page 104

We

element the strain is e(z), and at the other end it is e(x + Az) = e(x) + (Öe/ðr) Ar = e

(x) + (6°u/ðr”) Ar, and so the resultant force acting on the element is c(6°u/ðr") Ar.

We

**consider**the forces acting on an element of length Az. At one end of theelement the strain is e(z), and at the other end it is e(x + Az) = e(x) + (Öe/ðr) Ar = e

(x) + (6°u/ðr”) Ar, and so the resultant force acting on the element is c(6°u/ðr") Ar.

Page 579

F. MAGNETIC AND ELECTROSTATIC ENERGY We shall

magnetic energy, as the corresponding expressions for electric energy are

obtained by appropriate transcription. Our treatment is simple and rather naive,

but it ...

F. MAGNETIC AND ELECTROSTATIC ENERGY We shall

**consider**explicity onlymagnetic energy, as the corresponding expressions for electric energy are

obtained by appropriate transcription. Our treatment is simple and rather naive,

but it ...

Page 581

We

nucleus, the whole being placed in an inhomogeneous crystalline electric field.

We omit electron spin from the problem, as we are concerned here only with ...

We

**consider**a single electron with orbital quantum number L = 1 moving about anucleus, the whole being placed in an inhomogeneous crystalline electric field.

We omit electron spin from the problem, as we are concerned here only with ...

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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