Interactions of High Energy Particles with Nuclei |
From inside the book
Page 30
( The process of KK , ' regeneration given below is an example where we know ni's however ! ) The situation changes when we accept that diffractive production processes are weak compared to. 3 One must , however , keep in mind that in ...
( The process of KK , ' regeneration given below is an example where we know ni's however ! ) The situation changes when we accept that diffractive production processes are weak compared to. 3 One must , however , keep in mind that in ...
Page 32
... another target we can regenerate K , mesons because Ko and Ko interact differently with matter , they are absorbed differently . ( e.g. , K ° ( S = -1 ) + p — 4 ° ( S = -1 ) +7+ while Ko ( S = + 1 ) cannot produce Ao ) .
... another target we can regenerate K , mesons because Ko and Ko interact differently with matter , they are absorbed differently . ( e.g. , K ° ( S = -1 ) + p — 4 ° ( S = -1 ) +7+ while Ko ( S = + 1 ) cannot produce Ao ) .
Page 33
In order to measure these cross sections , one has to get off the forward direction where the transmission regeneration ( which comes from a coherent process whose coherence extends over the whole block of matter ) dominates .
In order to measure these cross sections , one has to get off the forward direction where the transmission regeneration ( which comes from a coherent process whose coherence extends over the whole block of matter ) dominates .
Page 34
Imf ( in fermis ) fron frop -3 for ~ 4 GeV / c 2 Ref ( in fermis ) -1 +1 From this picture it is clear that neutrons are much more effective in regeneration than protons ( the difference in absorption of K and Ko is much bigger in the ...
Imf ( in fermis ) fron frop -3 for ~ 4 GeV / c 2 Ref ( in fermis ) -1 +1 From this picture it is clear that neutrons are much more effective in regeneration than protons ( the difference in absorption of K and Ko is much bigger in the ...
Page 42
... Note that here the state | 0 , n ) is “ almost physical . ” More precisely : as far as strong interactions go , it is physical . The situation is very similar to that in the K1 - K , regeneration problem : we are expanding our ...
... Note that here the state | 0 , n ) is “ almost physical . ” More precisely : as far as strong interactions go , it is physical . The situation is very similar to that in the K1 - K , regeneration problem : we are expanding our ...
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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 |