Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Results 1-5 of 8
Page 2
... strong enough to insure the existence of multiple scattering ) . Hence we shall start with the very successful model of such processes : the Glauber model . 2. Description of Multiple Scattering 2.1 . General Remarks To construct the ...
... strong enough to insure the existence of multiple scattering ) . Hence we shall start with the very successful model of such processes : the Glauber model . 2. Description of Multiple Scattering 2.1 . General Remarks To construct the ...
Page 10
... strong inter- actions are mediated through vector fields ( analogous to the electromagnetic field ) one can expect the " principle of additivity of phase shifts " to be violated . 3. Elastic Scattering of Hadrons from Nuclei Let us go ...
... strong inter- actions are mediated through vector fields ( analogous to the electromagnetic field ) one can expect the " principle of additivity of phase shifts " to be violated . 3. Elastic Scattering of Hadrons from Nuclei Let us go ...
Page 19
... strong interactions were switched off ) and the strong interaction phase shift ( x , the phase shift we would get if the Coulomb interactions were switched off ; for x . we have the expression x . = Σ ; x ;. ) . This assumption is , of ...
... strong interactions were switched off ) and the strong interaction phase shift ( x , the phase shift we would get if the Coulomb interactions were switched off ; for x . we have the expression x . = Σ ; x ;. ) . This assumption is , of ...
Page 39
... in total agreement with the Bethe and Maximon formulae [ 34 ] for the high energy limit of the pair production cross section in a strong Coulomb field [ 35 ] . Example 2 : One particle exchange process : Drell and 39 AND ...
... in total agreement with the Bethe and Maximon formulae [ 34 ] for the high energy limit of the pair production cross section in a strong Coulomb field [ 35 ] . Example 2 : One particle exchange process : Drell and 39 AND ...
Page 42
... strong interactions go , it is physical . The situation is very similar to that in the K - K , regeneration problem : we are expanding our physical states into states which are " physical in their strong interactions . " Since we know ...
... strong interactions go , it is physical . The situation is very similar to that in the K - K , regeneration problem : we are expanding our physical states into states which are " physical in their strong interactions . " Since we know ...
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