Introduction to Solid State Physicsproblems after each chapter |
From inside the book
Results 1-3 of 62
Page 27
In the trigonal system a rhombohedron is usually chosen as the unit cell . The
lattice is primitive , but it is usually denoted by R , rather than P , so that we speak
of the trigonal R space lattice . Fig . 1.13 . Primitive translation vectors of the body
...
In the trigonal system a rhombohedron is usually chosen as the unit cell . The
lattice is primitive , but it is usually denoted by R , rather than P , so that we speak
of the trigonal R space lattice . Fig . 1.13 . Primitive translation vectors of the body
...
Page 164
M ELECTRONIC POLARIZABILITIES The total polarizability of an atom or ion
may usually be separated into three parts : 5 electronic , ionic , and orientational .
The electronic contribution arises from the displacement of electrons in an atom ...
M ELECTRONIC POLARIZABILITIES The total polarizability of an atom or ion
may usually be separated into three parts : 5 electronic , ionic , and orientational .
The electronic contribution arises from the displacement of electrons in an atom ...
Page 415
In some sintered ferrites the regions appear to be divided up in another fashion ,
with reversible rotation effective at low H. Closer examination reveals that in
weak fields the magnetization changes usually proceed by means of domain ...
In some sintered ferrites the regions appear to be divided up in another fashion ,
with reversible rotation effective at low H. Closer examination reveals that in
weak fields the magnetization changes usually proceed by means of domain ...
What people are saying - Write a review
We haven't found any reviews in the usual places.
Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
Copyright | |
17 other sections not shown
Other editions - View all
Common terms and phrases
alloys applied approximately associated atoms axis band boundary calculated cell chapter charge concentration condition conductivity consider constant crystal cubic density dependence determined dielectric diffusion direction discussion dislocation distribution domain effect elastic electric electron elements energy equal equation equilibrium experimental expression factor field force frequency function germanium give given heat capacity hexagonal holes important impurity increase interaction ionic ions lattice levels London magnetic magnetic field mass material measurements metals method motion normal observed obtained parallel particles Phys physics plane polarization positive possible potential problem properties range reference reflection region relation resistivity result room temperature rotation shown in Fig simple solid solution space space group specimen structure surface symmetry Table temperature theory thermal tion transition unit usually values vector volume wave zero zone