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Page 151
Furthermore , the atomic electrons possess intrinsic magnetic moments which cannot be expressed in terms of a current density . These moments can give rise to dipole fields which vary appreciably on the atomic scale of dimensions .
Furthermore , the atomic electrons possess intrinsic magnetic moments which cannot be expressed in terms of a current density . These moments can give rise to dipole fields which vary appreciably on the atomic scale of dimensions .
Page 368
For electrons in atoms the acceleration is caused by the screened Coulomb field ( 11.44 ) . ... called the Thomas factor ) , yielding 1 1 dV U S.L ( 11.56 ) 2m2c2 as the correct spin - orbit interaction energy for an atomic electron .
For electrons in atoms the acceleration is caused by the screened Coulomb field ( 11.44 ) . ... called the Thomas factor ) , yielding 1 1 dV U S.L ( 11.56 ) 2m2c2 as the correct spin - orbit interaction energy for an atomic electron .
Page 559
Consequently in an atomic or nuclear transition the lowest nonvanishing multipole will generally be the only one of importance . The ratio of transition probabilities for successive orders of either electric or magnetic multipoles of ...
Consequently in an atomic or nuclear transition the lowest nonvanishing multipole will generally be the only one of importance . The ratio of transition probabilities for successive orders of either electric or magnetic multipoles of ...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
TimeVarying Fields Maxwells Equations Con | 169 |
Copyright | |
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