Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 15
... factors of the colliding hadrons . This formula was used successfully to : ( i ) reproduce the proton charge form ... factor 1 - y ( b ) . Hence , the probability that the particle gets removed from the incident beam is 1— | 1 — y ( b ) ...
... factors of the colliding hadrons . This formula was used successfully to : ( i ) reproduce the proton charge form ... factor 1 - y ( b ) . Hence , the probability that the particle gets removed from the incident beam is 1— | 1 — y ( b ) ...
Page 22
... factors make Coulomb corrections insignificant in do DT / do . How important are the details of the target nucleus wave function ? Not very important . The most important are general characteristics : density distributions ( hence ...
... factors make Coulomb corrections insignificant in do DT / do . How important are the details of the target nucleus wave function ? Not very important . The most important are general characteristics : density distributions ( hence ...
Page 23
... factor to M = ( M ( △ ; 81 ... SA ) ) assuming the wave function to be in the form of a product of the c.m. wave function and the internal wave function . M = ( R ( r ) | exp ( i △ ⋅r ) | R ( r ) ) ( Þ 。( rı ′ . . . ra ′ ) | M ′ | Þ ...
... factor to M = ( M ( △ ; 81 ... SA ) ) assuming the wave function to be in the form of a product of the c.m. wave function and the internal wave function . M = ( R ( r ) | exp ( i △ ⋅r ) | R ( r ) ) ( Þ 。( rı ′ . . . ra ′ ) | M ′ | Þ ...
Page 24
Wiesław Czyż. Hence if we can factor out the c.m. wave function from the product = II ; ; ( r ; ) we can stick to calculating M with Yo but we have to multiply it by a correction factor : ( R ( r ) | exp ( i △ · r ) | R ( r ) ) −1 ...
Wiesław Czyż. Hence if we can factor out the c.m. wave function from the product = II ; ; ( r ; ) we can stick to calculating M with Yo but we have to multiply it by a correction factor : ( R ( r ) | exp ( i △ · r ) | R ( r ) ) −1 ...
Page 25
... factor exp ( R242 / 4A ) . For small A ( say A = 2 , 3 or 4 ) it can be a correction of as much as 2 orders of magnitude for A2 0.3 GeV2 . A few concluding remarks about the deuteron target . A lot of attention was concentrated on the ...
... factor exp ( R242 / 4A ) . For small A ( say A = 2 , 3 or 4 ) it can be a correction of as much as 2 orders of magnitude for A2 0.3 GeV2 . A few concluding remarks about the deuteron target . A lot of attention was concentrated on the ...
Common terms and phrases
absorption additivity of phase anomalous magnetic moment ú approximately assume attenuation b+½s beam Bureau of Standards coherent diffractive production collision Compton scattering compute Coulomb interactions Czyż d³r db exp i▲·b deuteron diagonalization diffractive production processes diffractive scattering discussed double scattering elastic scattering amplitude electromagnetic equation example excited experiments factor Feynman diagrams formula four-momentum Glauber model hadrons Hence high energy limit incident particle incident wave inelastic shadowing Interactions of High invariant mass K mesons multiple scattering National Bureau neutrino neutrons ññ Note nuclear matter nuclear targets nuclei nucleon obtained optical theorem parameters phase shifts photon photoproduction of vector physical pion production amplitude profiles quantum numbers regeneration Řº shadowing effects single scattering spin strongly interacting target nucleus total cross section vector meson VMD model wave function γν Σ Σ