Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 1
... problems related to the interactions of hadrons , photons , and electrons ( virtual photons ) with nuclei - we must choose a certain point of view which unifies all these problems . The common denominator which we shall emphasize is the ...
... problems related to the interactions of hadrons , photons , and electrons ( virtual photons ) with nuclei - we must choose a certain point of view which unifies all these problems . The common denominator which we shall emphasize is the ...
Page 7
... problem . We can also make the following remark : sometimes coupled channels can be decoupled by diagonalization . · A remark about “ decoupling " channels through a diagonalization procedure Start with a generalization ( to N channels ) ...
... problem . We can also make the following remark : sometimes coupled channels can be decoupled by diagonalization . · A remark about “ decoupling " channels through a diagonalization procedure Start with a generalization ( to N channels ) ...
Page 12
... problem from the point of view of a Glauber - like description of scattering of two composite objects . The formulae given below are interesting also because they may be used to analyze high energy nucleus - nucleus collisions ( which ...
... problem from the point of view of a Glauber - like description of scattering of two composite objects . The formulae given below are interesting also because they may be used to analyze high energy nucleus - nucleus collisions ( which ...
Page 18
... problem in more detail , one has to link it with diffractive production processes and we shall postpone such a discussion until our analysis of such processes . Here , let us make only the following points : ( i ) Diffractive production ...
... problem in more detail , one has to link it with diffractive production processes and we shall postpone such a discussion until our analysis of such processes . Here , let us make only the following points : ( i ) Diffractive production ...
Page 23
... problems . Let us introduce the transverse component of the c.m. vector r = 1 A 1⁄2 Sj , and the relative coordinates which are not independent any more : s1 = s ; -r , 8 , s ' + r A Ź s ; ' = 0 = 0 . The operator M ( A ; $ 1 ... SA ) ...
... problems . Let us introduce the transverse component of the c.m. vector r = 1 A 1⁄2 Sj , and the relative coordinates which are not independent any more : s1 = s ; -r , 8 , s ' + r A Ź s ; ' = 0 = 0 . The operator M ( A ; $ 1 ... SA ) ...
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