Classical Electrodynamics |
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Page 295
( t ) dt 2ka Jo The transmission coefficient increases more or less monotonically
as ka increases , with small oscillations superposed . For ka > 1 , the second form
in ( 9 . 109 ) can be used to obtain an asymptotic expression , T = 1 - zka - zlkas ...
( t ) dt 2ka Jo The transmission coefficient increases more or less monotonically
as ka increases , with small oscillations superposed . For ka > 1 , the second form
in ( 9 . 109 ) can be used to obtain an asymptotic expression , T = 1 - zka - zlkas ...
Page 446
69 ) , we find , after some calculation , the expression due to Fermi , ( ) = 2 ( ze
Resim * aK / ( 2 * a ) Ko ( ra ) ( \ dx / b > a TT v2 where 2 is given by ( 13 . 62 ) .
This result can be obtained more elegantly by calculating the electromagnetic
energy ...
69 ) , we find , after some calculation , the expression due to Fermi , ( ) = 2 ( ze
Resim * aK / ( 2 * a ) Ko ( ra ) ( \ dx / b > a TT v2 where 2 is given by ( 13 . 62 ) .
This result can be obtained more elegantly by calculating the electromagnetic
energy ...
Page 447
where we have used the dipole moment expression ( 13 . 19 ) . Assuming that the
second term is small , the imaginary part of 1 / € ( w ) can be readily calculated
and substituted into ( 13 . 70 ) . Then the integral over dw can be performed in the
...
where we have used the dipole moment expression ( 13 . 19 ) . Assuming that the
second term is small , the imaginary part of 1 / € ( w ) can be readily calculated
and substituted into ( 13 . 70 ) . Then the integral over dw can be performed in the
...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
RelativisticParticle Kinematics and Dynamics | 391 |
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