Interactions of High Energy Particles with Nuclei |
From inside the book
Page 1
Nevertheless , one still hopes to be able to learn something new , for example about short range nucleon correlation functions in target nuclei or about the presence of resonances in nuclear ground states [ 3 , 4 ] —just to name two ...
Nevertheless , one still hopes to be able to learn something new , for example about short range nucleon correlation functions in target nuclei or about the presence of resonances in nuclear ground states [ 3 , 4 ] —just to name two ...
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( Nonetheless there exists a motivation for belief in their existence : as in the case of photons interacting with nucleons — where the strongly interacting vector mesons seem to dominate - in the case of neutrino interactions — as was ...
( Nonetheless there exists a motivation for belief in their existence : as in the case of photons interacting with nucleons — where the strongly interacting vector mesons seem to dominate - in the case of neutrino interactions — as was ...
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and assuming that the particle goes through the target so fast that all the nucleons are ' frozen ' at certain positions , we get for the amplitude ik Msi = db ) 2 . l dru ... dor \ , * ( no ... ra ) sa ra ) | < ob exp ( ia.b ) x { 1- ...
and assuming that the particle goes through the target so fast that all the nucleons are ' frozen ' at certain positions , we get for the amplitude ik Msi = db ) 2 . l dru ... dor \ , * ( no ... ra ) sa ra ) | < ob exp ( ia.b ) x { 1- ...
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... y ) eikz transmitted wave : g ( x , y ) eik2 ( 1-4 ( x , y ) ) ( this is all under the assumption z « L ) . z 2 Let us construct the " shape of the shadow ” for a collection of scatterers ( nucleons in a nucleus ; see e.g. , fig .
... y ) eikz transmitted wave : g ( x , y ) eik2 ( 1-4 ( x , y ) ) ( this is all under the assumption z « L ) . z 2 Let us construct the " shape of the shadow ” for a collection of scatterers ( nucleons in a nucleus ; see e.g. , fig .
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( 3.2 ) 2 What kind of formulae would we have if the " ansatz " of additivity of phase shifts of the composite system ( 6 ) colliding with nucleons of ( a ) were valid ? Let us look at the profile of the jth nucleon : B B T ; ( d's II ...
( 3.2 ) 2 What kind of formulae would we have if the " ansatz " of additivity of phase shifts of the composite system ( 6 ) colliding with nucleons of ( a ) were valid ? Let us look at the profile of the jth nucleon : B B T ; ( d's II ...
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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 |
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