## Introduction to Solid State Physicsproblems after each chapter. |

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Page 4

If now we rotate a by an angle A, we get a new

cos A; av' = o sin A. If the lattice is invariant under the rotation A, the

must be of the form T, as in Eq. (1.3). The

If now we rotate a by an angle A, we get a new

**vector**a' with components ox' = ocos A; av' = o sin A. If the lattice is invariant under the rotation A, the

**vector**a' — amust be of the form T, as in Eq. (1.3). The

**vector**a' — a has the components ax' ...Page 50

The

long as the

from the origin in a given row in the reciprocal lattice corresponds to the nth order

...

The

**vector**r* (hkl) in the reciprocal lattice is in the same direction but n times aslong as the

**vector**corresponding to the true crystal plane. That is, the nth pointfrom the origin in a given row in the reciprocal lattice corresponds to the nth order

...

Page 545

The resulting strain pattern is that of the dislocation characterized jointly by the

boundary curve and the Burgers

one of a discrete set of lat tice

The resulting strain pattern is that of the dislocation characterized jointly by the

boundary curve and the Burgers

**vector**. It is clear that the Burgers**vector**must beone of a discrete set of lat tice

**vectors**that will allow the rewelding process to ...### What people are saying - Write a review

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### Contents

DIFFRACTION OF XRAYS BY CRYSTALS | 44 |

CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |

ELASTIC CONSTANTS OF CRYSTALS | 85 |

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absorption acceptors alkali alloy approximately atoms axes 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 levels low temperatures magnetic field metals molecules motion nearest neighbor normal observed orbital p-n junction paramagnetic particles phonons Phys physics plane polarizability polarization positive potential Proc recombination 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 transistor transition unit volume vacancies valence band values vector velocity wave functions wavelength x-ray zero