Interactions of High Energy Particles with Nuclei |
From inside the book
Page 38
Hence one can use the same technique to describe the processes on simple and composite ( e.g. , nuclei ) targets ( S4 ] . Relation of the above model to some well established techniques of describing diffractive dissociation .
Hence one can use the same technique to describe the processes on simple and composite ( e.g. , nuclei ) targets ( S4 ] . Relation of the above model to some well established techniques of describing diffractive dissociation .
Page 46
27 M ( 7V ) is given graphically below rum v In the high energy limit ( wo ) one can also describe this process as follows : the photon penetrates the nucleus up to a certain point where it converts into a V meson which scatters ...
27 M ( 7V ) is given graphically below rum v In the high energy limit ( wo ) one can also describe this process as follows : the photon penetrates the nucleus up to a certain point where it converts into a V meson which scatters ...
Page 51
Just to give some idea of how the results look , let us describe briefly the results of po photoproduction on deuterium ( R. L. Anderson et al . [ 39 ] ) and a DESY - MIT experiment ( H. Alvensleben et al .
Just to give some idea of how the results look , let us describe briefly the results of po photoproduction on deuterium ( R. L. Anderson et al . [ 39 ] ) and a DESY - MIT experiment ( H. Alvensleben et al .
Page 60
( From ( 5.5 ) one can see again that the " one step ” formula ( 5.3 ) is incapable of describing K1 - K , regeneration on nuclei ) . Let us go back to the general case of incoming particle 1 and outgoing particle 2.
( From ( 5.5 ) one can see again that the " one step ” formula ( 5.3 ) is incapable of describing K1 - K , regeneration on nuclei ) . Let us go back to the general case of incoming particle 1 and outgoing particle 2.
Page 61
( In the weak coupling case ” it is physically more accurate to describe the initial and final states as composed , approximately , of one and three particles , respectively . ) Note the following amusing point : Assuming | * ) to be in ...
( In the weak coupling case ” it is physically more accurate to describe the initial and final states as composed , approximately , of one and three particles , respectively . ) Note the following amusing point : Assuming | * ) to be in ...
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absorption additivity analysis approximately assume attenuation beam Bureau of Standards charge coherent collision complete components compute consider contribution corrections Coulomb Coulomb interactions coupling cross section db exp depend describe deuteron diffractive production processes discussed effects elastic scattering elastic scattering amplitude equation example excited existence exp ia.b experimental experiments expression fact factor field final formula forward given gives Glauber hadrons Hence high energy limit important incident particle inelastic initial Institute interactions introduce magnetic mass materials measurement momentum transfer multiple scattering National Bureau Note nuclear nuclear targets nuclei nucleon numbers objects obtained parameters phase shifts photon photoproduction physical position possible problem profiles shadowing single Standards step strong structure technical vector meson wave function
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 |