## Introduction to Solid State PhysicsNew edition of the most widely-used textbook on solid state physics in the world. Describes how the excitations and imperfections of actual solids can be understood with simple models that have firmly established scope and power. The foundation of this book is based on experiment, application and theory. Several significant advances in the field have been added including high temperature superconductors, quasicrystals, nanostructures, superlattices, Bloch/Wannier levels, Zener tunneling, light-emitting diodes and new magnetic materials. |

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Results 1-3 of 46

Page 6

_: We may arrange the origin, which we have called the associated lattice point,

so that 0 S xj, yj, zj S 1. Primitive Lattice Cell The parallelepiped defined by

primitive axes a1, a2, a3 is called a

type of ...

_: We may arrange the origin, which we have called the associated lattice point,

so that 0 S xj, yj, zj S 1. Primitive Lattice Cell The parallelepiped defined by

primitive axes a1, a2, a3 is called a

**primitive cell**(Fig. 5b). A**primitive cell**is atype of ...

Page 7

All other pairs shown of a1 and a2 may be taken as the primitive translation

vectors of the lattice. The parallelograms 1, 2, 3 are equal in area and any of

them could be taken as the

of a ...

All other pairs shown of a1 and a2 may be taken as the primitive translation

vectors of the lattice. The parallelograms 1, 2, 3 are equal in area and any of

them could be taken as the

**primitive cell**. The parallelogram 4 has twice the areaof a ...

Page 12

Table 2 Characteristics of cubic lattices' Simple Body-centered Face-centered

Volume, conventional cell a3 as (13 Lattice points per cell 1 2 4 Volume,

Table 2 Characteristics of cubic lattices' Simple Body-centered Face-centered

Volume, conventional cell a3 as (13 Lattice points per cell 1 2 4 Volume,

**primitive****cell**as ins tag Lattice points per unit volume 1/a3 2/as 4/all Number of nearest ...### What people are saying - Write a review

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### Contents

PERIODIC ARRAYS OF ATOMS | 3 |

INDEX SYSTEM FOR CRYSTAL PLANES | 12 |

NONIDEAL CRYSTAL STRUCTURES | 21 |

Copyright | |

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absolute zero alloys approximation atoms band edge Bloch Brillouin zone calculated Chapter charge collisions components conduction band conduction electrons crystal structure cubic deﬁned density dielectric function diffraction direction dislocation dispersion relation displacement effective mass elastic electric field electron concentration electron gas energy band energy gap equation equilibrium exciton experimental Fermi surface ferroelectric ferromagnetic ﬁeld Figure ﬁlled ﬁrst Fourier free atom free electron frequency germanium heat capacity hole impurity integral interaction ion cores lattice constant lattice point low temperatures magnetic field metals modes momentum motion nearest-neighbor normal optical orbitals oscillator particle phase phonon plane plasmons polarization positive potential energy primitive cell quantum reciprocal lattice vector resonance result scattering semiconductor shown in Fig silicon Solid state physics space specimen sphere spin superconducting Table theory thermal tion transition valence band values velocity volume wave wavefunction wavelength wavevector x-ray zone boundary zone scheme