Interactions of High Energy Particles with Nuclei |
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Page 7
Each infinitesimal step x ( z + Az ) – x ( z ) = iAzK ( 01.31 - idi.E10 , ) x ( 2 ) , x ( 2+ Az ) = eiA : K ( * ) x ( 2 ) , ) should be applied in order of increasing z's . That is what { ... } + means . In any case , the additivity ...
Each infinitesimal step x ( z + Az ) – x ( z ) = iAzK ( 01.31 - idi.E10 , ) x ( 2 ) , x ( 2+ Az ) = eiA : K ( * ) x ( 2 ) , ) should be applied in order of increasing z's . That is what { ... } + means . In any case , the additivity ...
Page 18
But as long as we construct the profiles of the target nucleus from profiles of elastic scattering , the processes like the one shown in figure 7 ( with excited states of the projectile present at intermediate steps ) are excluded .
But as long as we construct the profiles of the target nucleus from profiles of elastic scattering , the processes like the one shown in figure 7 ( with excited states of the projectile present at intermediate steps ) are excluded .
Page 35
0 Summing up : Our procedure for evaluating diffractive production in the limit of very high energy consists of two steps : ( i ) Find a " plausible ” model and identify the components of the incident and outgoing systems .
0 Summing up : Our procedure for evaluating diffractive production in the limit of very high energy consists of two steps : ( i ) Find a " plausible ” model and identify the components of the incident and outgoing systems .
Page 43
... -Ev rv Then M ( y = + ) = m ( = V ) πα Σ ( γ - V ) = V γν But νπα M ( 9V ) = M ( VV ) γν 4 Note that restricting the high energy photon - nucleus interaction to only vector meson interactions ( VMD model ) is a very drastic step .
... -Ev rv Then M ( y = + ) = m ( = V ) πα Σ ( γ - V ) = V γν But νπα M ( 9V ) = M ( VV ) γν 4 Note that restricting the high energy photon - nucleus interaction to only vector meson interactions ( VMD model ) is a very drastic step .
Page 55
Let us make this extension explicitly and obtain the so - called " one step ” model for diffractive production of hadrons in hadronnucleus collisions . In this “ one step ” process , the production takes place on a nucleon inside the ...
Let us make this extension explicitly and obtain the so - called " one step ” model for diffractive production of hadrons in hadronnucleus collisions . In this “ one step ” process , the production takes place on a nucleon inside the ...
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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 ground hadrons Hence high energy limit important incident particle inelastic initial Institute interactions introduce magnetic mass measurement momentum transfer multiple scattering National Bureau Note nuclear nuclear targets nuclei nucleon numbers objects obtained parameters phase shifts photon photoproduction physical position possible present problem profiles regeneration 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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