Interactions of High Energy Particles with Nuclei |
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Page 2
The expression 1 - eix ; ( b ) = y ; ( b ) is called the profile of the jth nucleon , incident particle collision . Assuming x ( b ) = = Σx ; ( b - s ; ) and assuming that the particle goes through the target so 2.
The expression 1 - eix ; ( b ) = y ; ( b ) is called the profile of the jth nucleon , incident particle collision . Assuming x ( b ) = = Σx ; ( b - s ; ) and assuming that the particle goes through the target so 2.
Page 7
... a1 and a2 generated by two sources of the elec- tromagnetic field ( at two different positions ) are , in general , noncommuting operators and there is no way of adding phase shifts ( or , equivalently , multiplying profiles ) .
... a1 and a2 generated by two sources of the elec- tromagnetic field ( at two different positions ) are , in general , noncommuting operators and there is no way of adding phase shifts ( or , equivalently , multiplying profiles ) .
Page 11
2rik When the incident wave already has a profile different from unity we get : incident wave : transmitted wave : g ( x , y ) eikz z g ( x , y ) eik ( 1 - y ( x , y ) ) ( this is all under the assumption z « < L ) .
2rik When the incident wave already has a profile different from unity we get : incident wave : transmitted wave : g ( x , y ) eikz z g ( x , y ) eik ( 1 - y ( x , y ) ) ( this is all under the assumption z « < L ) .
Page 12
... problem because there are experimental pro- jects under way ) . The geometry of the process is shown in figure 3 . 255 O A COMPONENTS ( b ) ( 0 ) O B COMPONENTS The profile describing the collision of two elements is : Yjk ( b ...
... problem because there are experimental pro- jects under way ) . The geometry of the process is shown in figure 3 . 255 O A COMPONENTS ( b ) ( 0 ) O B COMPONENTS The profile describing the collision of two elements is : Yjk ( b ...
Page 15
... η = Ξηι . Optical theorem and unitarity Let us first consider the " elementary " collisions ( whose scattering amplitude is determined by the profile ( b ) ) . As the wave passes a scatterer it gets modified by a factor 1 - y ( b ) ...
... η = Ξηι . Optical theorem and unitarity Let us first consider the " elementary " collisions ( whose scattering amplitude is determined by the profile ( b ) ) . As the wave passes a scatterer it gets modified by a factor 1 - y ( b ) ...
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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 |