## Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |

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**formula**plausible . One can use , e.g. , an optical description of attenuation of a wave penetrating a medium . One can also use some arguments based on approximate solutions of the wave equation of the incident particle interacting ... Page 4

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**formula**( 2.1 ) ; the reliability of this**formula**is of primary importance . The most complete analysis one can perform is presumably to employ the Watson multiple scattering theory , but we shall not present it here . In fact it is ... Page 12

... ( b − 8 , ® ) which is the profile for elastic scattering of ( b ) from the jth nucleon of ( a ) and a two - dimensional density p ( s ) = ƒ ** dz 4o * ( r ) ço ( r ) . 81 Then the additivity of phase shifts gives us the

... ( b − 8 , ® ) which is the profile for elastic scattering of ( b ) from the jth nucleon of ( a ) and a two - dimensional density p ( s ) = ƒ ** dz 4o * ( r ) ço ( r ) . 81 Then the additivity of phase shifts gives us the

**formula**121. Page 13

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**formula**( 3.2 ) sums over all intermediate excited states . For instance , the above contribution gives : ALL POSSIBLE EXCITED STATES Suppose we reject the intermediate excited states and take only the ground state as a possible inter ... Page 14

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**formula**( 3.2 ) this is a good place to discuss it a little further . As we have already said , it would be very interesting to test formulae of the type ( 3.2 ) against some experi- mental data . There is , however , very little data ...### 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