## 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 85

Page 36

Problem 1 is that the spacing d(hkl) between parallel lattice planes that are

normal to the direction G = hb, + kb2 + lb3 is d(hkl) = 27/|G|. Thus the result 2k : G

= G* may ...

**Equation**(23) is another statement of the Bragg condition (1). The result ofProblem 1 is that the spacing d(hkl) between parallel lattice planes that are

normal to the direction G = hb, + kb2 + lb3 is d(hkl) = 27/|G|. Thus the result 2k : G

= G* may ...

Page 184

G G k The wave

* = eX C(k)e" (26) R 2m G k k Each Fourier component must have the same

coefficient on both sides of the

G ...

G G k The wave

**equation**is obtained as the sum: 2 X. +-eco e" + X > UGC(k)e^**** = eX C(k)e" (26) R 2m G k k Each Fourier component must have the same

coefficient on both sides of the

**equation**. Thus (A. – e C(k) + 2 UCC(k - G)=0 . (27)G ...

Page 186

Thus exp(ik T) is the phase factor" by which a Bloch function is multiplied when

we make a crystal lattice translation T. • If the lattice potential vanishes, the

central

except C(k) ...

Thus exp(ik T) is the phase factor" by which a Bloch function is multiplied when

we make a crystal lattice translation T. • If the lattice potential vanishes, the

central

**equation**(27) reduces to (Ak - e)C(k) = 0, so that all C(k - G) are zeroexcept C(k) ...

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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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### Common terms and phrases

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