Introduction to Solid State Physicsproblems after each chapter |
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Page 10
ners of a unit cell , but it is clear that other two - fold axes are implicit in the pattern
. The pattern of symmetry elements is known as a space group , and a plan of a
unit of the complete space group p2 ( short symbol ) is shown in Fig . 1 . 6b .
ners of a unit cell , but it is clear that other two - fold axes are implicit in the pattern
. The pattern of symmetry elements is known as a space group , and a plan of a
unit of the complete space group p2 ( short symbol ) is shown in Fig . 1 . 6b .
Page 26
11 by a conventional unit cell of each . The conventional cells are not always
primitive , as sometimes a multiply primitive cell has a closer connection with the
symmetry elements than has a primitive cell . In the triclinic system the single
space ...
11 by a conventional unit cell of each . The conventional cells are not always
primitive , as sometimes a multiply primitive cell has a closer connection with the
symmetry elements than has a primitive cell . In the triclinic system the single
space ...
Page 313
3 ) V = a b X c = tao ; we see that this is correct because the unit cube of volume
ao contains two lattice points . The primitive translations a * , b * , c * of the
reciprocal lattice are given , according to ( 2 . 10 ) , by relations of the form b X c .
( 12 .
3 ) V = a b X c = tao ; we see that this is correct because the unit cube of volume
ao contains two lattice points . The primitive translations a * , b * , c * of the
reciprocal lattice are given , according to ( 2 . 10 ) , by relations of the form b X c .
( 12 .
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Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
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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 mass material measurements metals method motion normal observed obtained parallel particles Phys physics plane polarization positive possible potential present 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