Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Results 1-5 of 23
Page 2
... Assuming x ( b ) = = Σx ; ( b - s ; ) and assuming that the particle goes through the target so 2.
... Assuming x ( b ) = = Σx ; ( b - s ; ) and assuming that the particle goes through the target so 2.
Page 3
Wiesław Czyż. and assuming that the particle goes through the target so fast that all the nucleons are ' frozen ' at certain positions , we get for the amplitude Mfi = ik 27 / d3rı dr ... ray , * ( r ... ra ) | bexp ( iA + b ) × { 1 ...
Wiesław Czyż. and assuming that the particle goes through the target so fast that all the nucleons are ' frozen ' at certain positions , we get for the amplitude Mfi = ik 27 / d3rı dr ... ray , * ( r ... ra ) | bexp ( iA + b ) × { 1 ...
Page 12
... assume also that all particles have the same single particle wave functions . The ground state wave functions are ... assumed all profiles to be identical and introduced B ï ; ( b ) = [ đ3rı ¢ o® ) * ( r , ® ) ¢ o® ( r , ® ) Y ; t ( b ...
... assume also that all particles have the same single particle wave functions . The ground state wave functions are ... assumed all profiles to be identical and introduced B ï ; ( b ) = [ đ3rı ¢ o® ) * ( r , ® ) ¢ o® ( r , ® ) Y ; t ( b ...
Page 14
... assume that all y's are the same . One gets this formula trivially from M = ik 2π db exp ( i △ · b ) | [ 1- ( 1- S ... assumes that y ( b ) is a very narrow function of b ( hence the components of the two hadrons are very small ) we can ...
... assume that all y's are the same . One gets this formula trivially from M = ik 2π db exp ( i △ · b ) | [ 1- ( 1- S ... assumes that y ( b ) is a very narrow function of b ( hence the components of the two hadrons are very small ) we can ...
Page 19
... assume that , in the high energy limit , the total phase shift is the sum of the Coulomb phase shift ( xe , the phase shift one would get if the strong interactions were switched off ) and the strong interaction phase shift ( x , the ...
... assume that , in the high energy limit , the total phase shift is the sum of the Coulomb phase shift ( xe , the phase shift one would get if the strong interactions were switched off ) and the strong interaction phase shift ( x , 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