Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
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Page 1
... inelastic electron - nucleus scattering , ( 7 ) Shadowing effects in neutrino reactions on nuclei . Key words : Diffractive production ; diffractive scattering ; Glauber model ; hadronic components of photons ; high energy scattering ...
... inelastic electron - nucleus scattering , ( 7 ) Shadowing effects in neutrino reactions on nuclei . Key words : Diffractive production ; diffractive scattering ; Glauber model ; hadronic components of photons ; high energy scattering ...
Page 18
... inelastic screening ( or inelastic shadowing ) phenomenon [ 47 ] . In order to include them we have to ascribe some kind of structure to the incident particle . Earlier in these notes we gave some examples of such cases . To analyze ...
... inelastic screening ( or inelastic shadowing ) phenomenon [ 47 ] . In order to include them we have to ascribe some kind of structure to the incident particle . Earlier in these notes we gave some examples of such cases . To analyze ...
Page 28
... inelastic processes : ( experiments seem to indicate that the differential cross sections depend weakly on energy ) γρ π → 5π p → n + π on nucleons or nuclei . K - Kπ , KππT etc. The nucleon and nuclear targets supplement each other ...
... inelastic processes : ( experiments seem to indicate that the differential cross sections depend weakly on energy ) γρ π → 5π p → n + π on nucleons or nuclei . K - Kπ , KππT etc. The nucleon and nuclear targets supplement each other ...
Page 29
... inelastic scattering amplitudes . Since the transmitted wave is = n , the wave which goes into scattering and production is ¥ n = nyyλeln + λinelnxe ; But hence ¥ 1 = Ny ¥ n — N2 ¥ ¤ × ¢ z ; λel = ny2 , λinel = -・ nzny . Geometrical ...
... inelastic scattering amplitudes . Since the transmitted wave is = n , the wave which goes into scattering and production is ¥ n = nyyλeln + λinelnxe ; But hence ¥ 1 = Ny ¥ n — N2 ¥ ¤ × ¢ z ; λel = ny2 , λinel = -・ nzny . Geometrical ...
Page 31
... inelastic amplitude ( X ; | T | X ; ) = ( 1 — ni ) ei ; — ( 1 — nj ) E ij ( 4.4 ) is proportional to the difference between the absorption of the produced particle and the absorption of the incident particle . One still faces the ...
... inelastic amplitude ( X ; | T | X ; ) = ( 1 — ni ) ei ; — ( 1 — nj ) E ij ( 4.4 ) is proportional to the difference between the absorption of the produced particle and the absorption of the incident particle . One still faces the ...
Common terms and phrases
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