Interactions of High Energy Particles with Nuclei |
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Page 1
Of course , we cannot cover all 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 .
Of course , we cannot cover all 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 .
Page 7
So , we have to deal with a coupled channels problem . We can make the following remark : sometimes coupled channels can be decoupled by diagonalization . . A remark about " decoupling " channels through ...
So , we have to deal with a coupled channels problem . We can make the following remark : sometimes coupled channels can be decoupled by diagonalization . . A remark about " decoupling " channels through ...
Page 12
We can also have a look at this 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 ...
We can also have a look at this 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 ...
Page 18
To analyze this 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 : a ( i ) ...
To analyze this 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 : a ( i ) ...
Page 23
In the case of more complicated targets the situation is much more involved and often leads to some serious computational problems . Let us introduce the transverse component of the c.m. vector ...
In the case of more complicated targets the situation is much more involved and often leads to some serious computational problems . Let us introduce the transverse component of the c.m. vector ...
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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