Interactions of High Energy Particles with Nuclei |
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Page 1
... and diffractive excitation , ( 5 ) Diffractive production of hadrons in hadron - nucleon collisions , ( 6 ) Shadowing effects in inelastic electron - nucleus scattering , ( 7 ) Shadowing effects in neutrino reactions on nuclei .
... and diffractive excitation , ( 5 ) Diffractive production of hadrons in hadron - nucleon collisions , ( 6 ) Shadowing effects in inelastic electron - nucleus scattering , ( 7 ) Shadowing effects in neutrino reactions on nuclei .
Page 18
O O O O They are the source of the so - called inelastic screening ( or inelastic shadowing ) phenomenon [ 47 ] . In order to include them we have to ascribe some kind of structure to the incident particle . Earlier in these notes we ...
O O O O They are the source of the so - called inelastic screening ( or inelastic shadowing ) phenomenon [ 47 ] . In order to include them we have to ascribe some kind of structure to the incident particle . Earlier in these notes we ...
Page 28
... Compton scattering , etc. in hadron physics ; all kinds of elastic hadron - hadron scattering do ( experiments seem to indicate that the = f ( ) differential cross sections depend weakly DA ? on energy ) inelastic processes : 7 - sp ...
... Compton scattering , etc. in hadron physics ; all kinds of elastic hadron - hadron scattering do ( experiments seem to indicate that the = f ( ) differential cross sections depend weakly DA ? on energy ) inelastic processes : 7 - sp ...
Page 29
Let us compute the elastic and inelastic scattering amplitudes . Since the transmitted wave is y = n , V , the wave which goes into scattering and production is ry - 4 = n ,, = ley + Aineinge , But Vy = n , Yn - nzYnyez ; hence 1 λο1 ...
Let us compute the elastic and inelastic scattering amplitudes . Since the transmitted wave is y = n , V , the wave which goes into scattering and production is ry - 4 = n ,, = ley + Aineinge , But Vy = n , Yn - nzYnyez ; hence 1 λο1 ...
Page 31
... zero zero = ( 1-7 ; 8 ; teji ( 1-7 ; ) - Eji ( 1 - ni ) . In this approximation ( Til T | 1i ) = 1 - mi = 2 Hence the absorption parameters ni are determined by elastic scattering of real particles . The inelastic amplitude ( il T | ...
... zero zero = ( 1-7 ; 8 ; teji ( 1-7 ; ) - Eji ( 1 - ni ) . In this approximation ( Til T | 1i ) = 1 - mi = 2 Hence the absorption parameters ni are determined by elastic scattering of real particles . The inelastic amplitude ( il T | ...
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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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