Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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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 analysis approximately assume attenuation beam coherent collision complete components compute consider contribution corrections Coulomb Coulomb interactions coupling cross section db exp db exp i▲·b depend describe deuteron diffractive production processes discussed effects elastic scattering elastic scattering amplitude equation example excited existence experimental experiments expression fact factor field final formula forward given gives Glauber ground hadrons Hence high energy limit important incident particle inelastic initial Institute interactions introduce magnetic mass measurement momentum transfer multiple scattering Note nuclear nuclear targets nuclei nucleon numbers objects obtained parameters phase shifts photon photoproduction physical position possible problem profiles regeneration shadowing single Standards step strong structure technical vector meson wave function weak
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 |