固态物理学 第2卷
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作者帕特森(James？D.Patterson) 著作
出版社世界图书出版公司
ISBN9787510029769
出版时间2010-12
装帧平装
开本其他
定价49元
货号11671674
上书时间2024-11-24
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作者简介
作者：（美国）帕特森（James D.Patterson） （美国）Bernard C.Bailey
目录
Crystal Binding and Structure
1.1 Classification of Solids by Binding Forces （B）
1.1.1 Molecular Crystals and the van der Waals Forces （B）
1.1.2 Ionic Crystals and Born-Mayer Theory （B）
1.1.3 Metals and Wigner-Seitz Theory （B）
1.1.4 Valence Crystals and Heitler-London Theory （B）
1.1.5 Comment on Hydrogen-Bonded Crystals （B）
1.2 Group Theory and Crystallography
1.2.1 Definition and Simple Properties of Groups （AB）
1.2.2 Examples of Solid-State Symmetry Properties （B）
1.2.3 Theorem: No Five-fold Symmetry （B）
1.2.4 Some Crystal Structure Terms and Nonderived Facts （B）
1.2.5 List of Crystal Systems and Bravais Lattices （B）
1.2.6 Schoenflies and International Notation for Point Groups （A）
1.2.7 Some Typical Crystal Structures （B）
1.2.8 Miller Indices （B）
1.2.9 Bragg and yon Lane Diffraction （AB）
Problems
2 Lattice Vibrations and Thermal Properties
2.1 The Born-Oppenheimer Approximation （A）
2.2 One-Dimensional Lattices （B）
2.2.1 Classical Two-Atom Lattice with Periodic Boundary Conditions （B）
2.2.2 Classical, Large, Perfect Monatomic Lattice,and Introduction to Brillouin Zones （B）
2.2.3 Specific Heat of Linear Lattice （B）
2.2.4 Classical Diatomic Lattices: Optic and Acoustic Modes （B）
2.2.5 Classical Lattice with Defects （B）
2.2.6 Quantum-Mechanical Linear Lattice （B）
2.3 Three-Dimensional Lattices
2.3.1 Direct and Reciprocal Lattices and Pertinent Relations （B）
2.3.2 Quantum-Mechanical Treatment and Classical
Calculation of the Dispersion Relation （B）
2.3.3 The Debye Theory of Specific Heat （B）
2.3.4 Anharmonic Terms in The Potential /The Gruneisen Parameter （A）
2.3.5 Wave Propagation in an Elastic Crystalline Continuum（MET, MS）
Problems
3 Electrons in Periodic Potentials
3.1 Reduction to One-Electron Problem
3.1.1 The Variational Principle （B）
3.1.2 The Hartree Approximation （B）
3.1.3 The Hartree――Fock Approximation （A）
3.1.4 Coulomb Correlations and the Many-Electron Problem （A）
3.1.5 Density Functional Approximation （A）
3.2 One-Electron Models
3.2.1 The Kronig-Penney Model （B）
3.2.2 The Free-Electron or Quasifree-Eiectron Approximation （B）
3.2.3 The Problem of One Electron in a Three-Dimensional Periodic Potential
3.2.4 Effect of Lattice Defects on Electronic States in Crystals （A）
Problems
4 The Interaction of Electrons and Lattice Vibrations
4.1 Particles and Interactions of Solid-state Physics （B）
4.2 The Phonon-Phonon Interaction （B）
4.2.1 Anharmonic Terms in the Hamiltonian （B）
4.2.2 Normal and Umklapp Processes （B）
4.2.3 Comment on Thermal Conductivity （B）
4.3 The Electron-Phonon Interaction
4.3.1 Form of the Hamiltonian （B）
4.3.2 Rigid-Ion Approximation （B）
4.3.3 The Polaron as a Prototype Quasiparticle （A）
4.4 Brief Comments on Electron-Electron Interactions （B）
……
5 metals,Alloys,and the Fermi Surface
6 Semiconductors
7 Magnetism,Magnons,and Magnetic Resonance
8 Superconductivity
9 Optical Properties of Solids
11 Defects in Solids
12 Current Topics in Solid Condensed-Matter Physics
Appendices
Bibliography
Index
内容摘要
《固态物理学(第2卷)》主要内容简介：Semiconductors、Magnetism,Magnons,and Magnetic Resonance、Superconductivity、Optical Properties of Solids、Defects in Solids、Current Topics in Solid Condensed-Matter Physics等。
主编推荐
《固态物理学(第2卷)》由世界图书出版公司出版。
精彩内容
hapter
1
was
concerned
with
the
binding
forces
in
crystals
and
with
the
mannerin
which
atoms
were
arranged.
Chapter
1
defined,
in
effect,
the
universe
withwhich
we
will
be
concerned.
We
now
begin
discussing
the
elements
of
this
uni-verse
with
which
we
interact.
Perhaps
the
most
interesting
of
these
elements
arethe
internal
energy
excitation
modes
of
the
crystals.
The
quanta
of
these
modes
arethe
"particles"
of
the
solid.
This
chapter
is
primarily
devoted
to
a
particular
typeof
internal
mode
-
the
lattice
vibrations.
The
lattice
introduced
in
Chap.
1,
as
we
already
mentioned,
is
not
a
static
struc-ture.
At
any
finite
temperature
there
will
be
thermal
vibrations.
Even
at
absolutezero,
according
to
quantum
mechanics,
there
will
be
zero-point
vibrations.
As
wewill
discuss,
these
lattice
vibrations
can
be
described
in
terms
of
normal
modesdescribing
the
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