Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Results 1-5 of 16
Page 1
... multiple scattering and shadowing processes inside of the target nuclei . An effort is made to develop a unified way of treating nuclear interactions of particles which are either hadrons or exhibit some hadronic components in such ...
... multiple scattering and shadowing processes inside of the target nuclei . An effort is made to develop a unified way of treating nuclear interactions of particles which are either hadrons or exhibit some hadronic components in such ...
Page 2
... multiple scattering process of strongly interacting particles inside of nuclear matter ( or more generally : just a multiple scattering process with forces strong enough to insure the existence of multiple scattering ) . Hence we shall ...
... multiple scattering process of strongly interacting particles inside of nuclear matter ( or more generally : just a multiple scattering process with forces strong enough to insure the existence of multiple scattering ) . Hence we shall ...
Page 4
... multiple scattering theory , but we shall not present it here . In fact it is amazing that ( 2.1 ) works so well . Even in the conceptually simplest cases of rela- tivistic potential scattering one can give examples in which it breaks ...
... multiple scattering theory , but we shall not present it here . In fact it is amazing that ( 2.1 ) works so well . Even in the conceptually simplest cases of rela- tivistic potential scattering one can give examples in which it breaks ...
Page 21
... multiple scattering description ) . - 00 = From this expression ( 3.7 ) one can see that the interplay of xc ( b ) and § ( b ) is , in this optical limit , determined by the size and sign of an and a ,. Some calculations were done [ 15 ] ...
... multiple scattering description ) . - 00 = From this expression ( 3.7 ) one can see that the interplay of xc ( b ) and § ( b ) is , in this optical limit , determined by the size and sign of an and a ,. Some calculations were done [ 15 ] ...
Page 24
... ( A ) = ik ( R2 + 2a ) exp R2A2 A 1 ( 1 - ia ) exp [ - 1 ( ~~ ) ≤ ( ^ ) <‹ - » » } [ z ; @ = 2 ] • [ − ¦ ( R2 + 20 ) a3 ] 4A ( -1 ) +1 j ( R2 + 2a ) 2π 4j Many general features of the multiple scattering are included in 24.
... ( A ) = ik ( R2 + 2a ) exp R2A2 A 1 ( 1 - ia ) exp [ - 1 ( ~~ ) ≤ ( ^ ) <‹ - » » } [ z ; @ = 2 ] • [ − ¦ ( R2 + 20 ) a3 ] 4A ( -1 ) +1 j ( R2 + 2a ) 2π 4j Many general features of the multiple scattering are included in 24.
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