Interactions of High Energy Particles with Nuclei |
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Page 13
For instance , we can extract from ( 3.2 ) the following contribution of the second order dør , Øço ) * ( 77 % ) yu ( b - 8,6 ) +5 . ( ) ) y21 ( b - 8,6 ) +32 ( ) ço ( ra ) ( ) - = / PorWdor ( 8 ) poca ) * ( ro ) yı ( b – 8,6 + 52 ...
For instance , we can extract from ( 3.2 ) the following contribution of the second order dør , Øço ) * ( 77 % ) yu ( b - 8,6 ) +5 . ( ) ) y21 ( b - 8,6 ) +32 ( ) ço ( ra ) ( ) - = / PorWdor ( 8 ) poca ) * ( ro ) yı ( b – 8,6 + 52 ...
Page 14
So , the Chou & Yang [ 13 ] limit A , B looses all excited state contributions and becomes ( 3.4 ) . Equation ( 3.4 ) gives the well - known " droplet model " [ 13 ] elastic scattering amplitude of two composite objects whose hadronic ...
So , the Chou & Yang [ 13 ] limit A , B looses all excited state contributions and becomes ( 3.4 ) . Equation ( 3.4 ) gives the well - known " droplet model " [ 13 ] elastic scattering amplitude of two composite objects whose hadronic ...
Page 16
... 1-11- ( T ) | 2 gives the probability ( at the impact parameter b ) of losing the incident particle from the elastic channel . It is convenient however to split the second term into two physically different contributions : 16.
... 1-11- ( T ) | 2 gives the probability ( at the impact parameter b ) of losing the incident particle from the elastic channel . It is convenient however to split the second term into two physically different contributions : 16.
Page 17
split the second term into two physically different contributions : | < b [ 2 Re ( r ) – [ { r } / # ] = [ [ < r + r ) – 1 ( T ) | : ] = ODT + | dob [ 2 Re ( T ) – ( + r ) ] = O PROD = Interpretation The first contribution ( opt ) comes ...
split the second term into two physically different contributions : | < b [ 2 Re ( r ) – [ { r } / # ] = [ [ < r + r ) – 1 ( T ) | : ] = ODT + | dob [ 2 Re ( T ) – ( + r ) ] = O PROD = Interpretation The first contribution ( opt ) comes ...
Page 18
If this is so , then the three contributions to otot discussed above do approximately exhaust the list of processes contributing to elastic scattering . From our discussion of the components of otot ( oel , odt , O PROD ) it follows ...
If this is so , then the three contributions to otot discussed above do approximately exhaust the list of processes contributing to elastic scattering . From our discussion of the components of otot ( oel , odt , O PROD ) it follows ...
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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 |