Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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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 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 |