Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Page 1
... nucleon collisions , ( 6 ) Shadowing effects in inelastic electron - nucleus scattering , ( 7 ) Shadowing effects in neutrino reactions on nuclei . Key words : Diffractive production ; diffractive scattering ; Glauber model ; hadronic ...
... nucleon collisions , ( 6 ) Shadowing effects in inelastic electron - nucleus scattering , ( 7 ) Shadowing effects in neutrino reactions on nuclei . Key words : Diffractive production ; diffractive scattering ; Glauber model ; hadronic ...
Page 2
... nucleon : f ; ( 8 ) = ik 11⁄2 / db exp ( i △ · b ) { 1— exp [ ix ; ( b − s ; ) ] } , where k is the momentum of ... nucleon elastic scat- tering amplitude . The expression 1 - eix ; ( b ) = y ; ( b ) is called the profile of the jth ...
... nucleon : f ; ( 8 ) = ik 11⁄2 / db exp ( i △ · b ) { 1— exp [ ix ; ( b − s ; ) ] } , where k is the momentum of ... nucleon elastic scat- tering amplitude . The expression 1 - eix ; ( b ) = y ; ( b ) is called the profile of the jth ...
Page 3
... nucleons are ' frozen ' at certain positions , we get for the amplitude Mfi = ik 27 / d3rı dr ... ray , * ( r ... ra ) | bexp ( iA + b ) × { 1 - exp [ Σx ; ( b − j ; ) ] } ¥ , ( r1 . . . r △ ) ik = 27 db exp ( iA.b ) d [ dr ...
... nucleons are ' frozen ' at certain positions , we get for the amplitude Mfi = ik 27 / d3rı dr ... ray , * ( r ... ra ) | bexp ( iA + b ) × { 1 - exp [ Σx ; ( b − j ; ) ] } ¥ , ( r1 . . . r △ ) ik = 27 db exp ( iA.b ) d [ dr ...
Page 11
... ( nucleons in a nucleus ; see e.g. , fig . 1 ) : The incident wave : after the first collision : after the second collision : etc. ik z e [ 1 - y1 ( b - sı ) ] e ik z [ 1-2 ( b - S2 ) ] [ 1 - y1 ( b - s1 ) ] e ik z The ' shape of the ...
... ( nucleons in a nucleus ; see e.g. , fig . 1 ) : The incident wave : after the first collision : after the second collision : etc. ik z e [ 1 - y1 ( b - sı ) ] e ik z [ 1-2 ( b - S2 ) ] [ 1 - y1 ( b - s1 ) ] e ik z The ' shape of the ...
Page 12
... nucleons of ( a ) were valid ? Let us look at the profile of the jth nucleon : 1 ; ( b ) = √ d2s16 ) ... B d2SÅ ( b ) II p ) ( 81 ) | 1- = 1 − ( 1 − ỹ ; ( b ) ) B , = - เ where we assumed all profiles to be identical and introduced B ...
... nucleons of ( a ) were valid ? Let us look at the profile of the jth nucleon : 1 ; ( b ) = √ d2s16 ) ... B d2SÅ ( b ) II p ) ( 81 ) | 1- = 1 − ( 1 − ỹ ; ( b ) ) B , = - เ where we assumed all profiles to be identical and introduced B ...
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