Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 3
... initial and final wave functions of the target nucleus . Yi , ( 2.1 ) One can produce many arguments which make this important formula plausible . One can use , e.g. , an optical description of attenuation of a wave penetrating a medium ...
... initial and final wave functions of the target nucleus . Yi , ( 2.1 ) One can produce many arguments which make this important formula plausible . One can use , e.g. , an optical description of attenuation of a wave penetrating a medium ...
Page 18
... initial one - a very complex process in which the whole of the nucleus must take part ( hence it occurs with small probability ) . ( iii ) Hence " inelastic shadowing " stands a good chance to contribute little ( a few percent ) to the ...
... initial one - a very complex process in which the whole of the nucleus must take part ( hence it occurs with small probability ) . ( iii ) Hence " inelastic shadowing " stands a good chance to contribute little ( a few percent ) to the ...
Page 27
... initial and final states , we exclude , by doing this , any possible relativistic deformations of the recoiling target ( we are still discussing only elastic processes ) . For large momentum transfers ( A2 / M2 ~ 1 ) this is probably ...
... initial and final states , we exclude , by doing this , any possible relativistic deformations of the recoiling target ( we are still discussing only elastic processes ) . For large momentum transfers ( A2 / M2 ~ 1 ) this is probably ...
Page 35
... initial and final states . ) As long as the time of the passage through ( or the interaction with ) the target is T << 2p M2 — M * 2 › we can consider the states to be degenerate because their relative phase factor during the collision ...
... initial and final states . ) As long as the time of the passage through ( or the interaction with ) the target is T << 2p M2 — M * 2 › we can consider the states to be degenerate because their relative phase factor during the collision ...
Page 56
... initial ( one pion ) and the final ( 3 states ) . Let us repeat the arguments again . 1 Initial state = + Final state = 2 2 small admixture = | Ĭ ) + d | 2 ) 1 + - = | 2 ) —d * | ĩ ) small admixture ( the orthogonality condition ...
... initial ( one pion ) and the final ( 3 states ) . Let us repeat the arguments again . 1 Initial state = + Final state = 2 2 small admixture = | Ĭ ) + d | 2 ) 1 + - = | 2 ) —d * | ĩ ) small admixture ( the orthogonality condition ...
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