Interactions of High Energy Particles with Nuclei |
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The result of this cooperation is reflected , however , not only in published papers , but in numerous unpublished notes as well as in these lectures themselves . L. C. Maximon Interactions of ...
The result of this cooperation is reflected , however , not only in published papers , but in numerous unpublished notes as well as in these lectures themselves . L. C. Maximon Interactions of ...
Page 1
In these notes the interactions of various different particles with nuclear targets are to be considered . Of course , we cannot cover all problems related to the interactions of hadrons , photons , and electrons ( virtual photons ) ...
In these notes the interactions of various different particles with nuclear targets are to be considered . Of course , we cannot cover all problems related to the interactions of hadrons , photons , and electrons ( virtual photons ) ...
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... ( 1 + az ) and get ( note that ( 1 + az ) ( 1 - a3 ) = azo = 0 ) 0 = [ - i5 ( 1 + as ) as • Va = iX5 ( 1 + as ) as id + % ( 1 + a ) $ = a +12 1 Bm дz -KY2 ( 1 + az ) ( 2.B - ia • E ) + eVY2 ( 1 + az ) 4 .
... ( 1 + az ) and get ( note that ( 1 + az ) ( 1 - a3 ) = azo = 0 ) 0 = [ - i5 ( 1 + as ) as • Va = iX5 ( 1 + as ) as id + % ( 1 + a ) $ = a +12 1 Bm дz -KY2 ( 1 + az ) ( 2.B - ia • E ) + eVY2 ( 1 + az ) 4 .
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... дг = m 1 Note that " compositeness " of the incident particle is responsible for the existence of more than one channel . For instance , the presence of an anomalous magnetic moment can be looked upon as a mark of " compositeness .
... дг = m 1 Note that " compositeness " of the incident particle is responsible for the existence of more than one channel . For instance , the presence of an anomalous magnetic moment can be looked upon as a mark of " compositeness .
Page 8
0 , -ix - iy ) V ' ( r ) Q ( b , z ) = K r i ( x + iy ) , 0 Note that since the z dependence is outside the spinor matrix this does commute at different z's : [ Q ( b , z ) , A ( 6,2 ' ) ] = 0 . Suppose , however , we have two sources ...
0 , -ix - iy ) V ' ( r ) Q ( b , z ) = K r i ( x + iy ) , 0 Note that since the z dependence is outside the spinor matrix this does commute at different z's : [ Q ( b , z ) , A ( 6,2 ' ) ] = 0 . Suppose , however , we have two sources ...
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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 |
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