Interactions of High Energy Particles with Nuclei |
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Page 2
The expression 1- eix ; ( b ) = Yi ( 6 ) is called the profile of the jth nucleon , incident particle collision . Assuming x ( b ) = Ï xi ( b - 8 ; ) ) and assuming that the particle goes through the target so.
The expression 1- eix ; ( b ) = Yi ( 6 ) is called the profile of the jth nucleon , incident particle collision . Assuming x ( b ) = Ï xi ( b - 8 ; ) ) and assuming that the particle goes through the target so.
Page 5
Thus , finally , we find a [ -ig + eV – KB ( 21 • B. - ia • El ) p = 0 . ( = . ( 2.4 ) дz So , if the anamalous magnetic moment K = 0 , we end up with an expression which is virtually the same as in the case of the Schrödinger equation ...
Thus , finally , we find a [ -ig + eV – KB ( 21 • B. - ia • El ) p = 0 . ( = . ( 2.4 ) дz So , if the anamalous magnetic moment K = 0 , we end up with an expression which is virtually the same as in the case of the Schrödinger equation ...
Page 15
Hence , the probability that the particle gets removed from the incident beam is 1-11 - ( 6 ) 12 = 2 Rey ( 6 ) – 10 ( 6 ) | 2 ( at the impact parameter b ) . Notice that here we use the same expression as - in the following paragraphs ...
Hence , the probability that the particle gets removed from the incident beam is 1-11 - ( 6 ) 12 = 2 Rey ( 6 ) – 10 ( 6 ) | 2 ( at the impact parameter b ) . Notice that here we use the same expression as - in the following paragraphs ...
Page 19
... the strong interaction phase shift ( xa , the phase shift we would get if the Coulomb interactions were switched off ; for x . we have the expression x : = Eixi ) . This assumption is , of course , obvious in potential scattering .
... the strong interaction phase shift ( xa , the phase shift we would get if the Coulomb interactions were switched off ; for x . we have the expression x : = Eixi ) . This assumption is , of course , obvious in potential scattering .
Page 20
( 120 ) n exp [ -in In ( 42 / 4k2 ) ] e2100 Ao / 2k where n = Ze / v , = 0o = arg 1 ( 1 + in ) . and hence we get the convergent expression for the complete amplitude by adding and subtracting a Coulomb point charge amplitude : M = ik ...
( 120 ) n exp [ -in In ( 42 / 4k2 ) ] e2100 Ao / 2k where n = Ze / v , = 0o = arg 1 ( 1 + in ) . and hence we get the convergent expression for the complete amplitude by adding and subtracting a Coulomb point charge amplitude : M = ik ...
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Bibliographic information
| Title | Interactions of High Energy Particles with Nuclei Volume 139 of NBS monograph |
| Author | Wiesław Czyż |
| Publisher | National Bureau of Standards, 1975 |
| Original from | the University of Michigan |
| Digitized | 21 Nov 2007 |
| Length | 69 pages |
| Export Citation | BiBTeX EndNote RefMan |