## 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 70

Page 35

Crystal specimen k i 0 t i b Incident beam u go llgr eam ear, ' Figure 6 The difl'

erence in path length of the incident wave k at the points O, r is r sin up, and the

difference in

diffracted ...

Crystal specimen k i 0 t i b Incident beam u go llgr eam ear, ' Figure 6 The difl'

erence in path length of the incident wave k at the points O, r is r sin up, and the

difference in

**phase**angle is (2rrr sin sp)/A, which is equal to k - r. For thediffracted ...

Page 369

(55) We see by integration of (55) that with a dc voltage across the junction the

relative

superconducting current is given by (47) with (56) for the

(55) We see by integration of (55) that with a dc voltage across the junction the

relative

**phase**of the probability amplitudes vary as 6(t) = 6(0) - (2eVt/h). (56) Thesuperconducting current is given by (47) with (56) for the

**phase**: J = Jo sin [ö(0) ...Page 615

g m E-' W 1 4(1) an 1 200 I I Figure 4 Equilibrium diagram of

-zinc alloy system. The a

and 1; are both hcp, but e has a c/a ratio near 1.56 and 1; (for pure Zn) has c/a ...

g m E-' W 1 4(1) an 1 200 I I Figure 4 Equilibrium diagram of

**phases**in the copper-zinc alloy system. The a

**phase**is fcc; B and B' are bcc; y is a complex structure; eand 1; are both hcp, but e has a c/a ratio near 1.56 and 1; (for pure Zn) has c/a ...

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### Contents

PERIODIC ARRAYS OF ATOMS | 3 |

INDEX SYSTEM FOR CRYSTAL PLANES | 12 |

NONIDEAL CRYSTAL STRUCTURES | 21 |

Copyright | |

26 other sections not shown

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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