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

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**factors**of the colliding hadrons . This formula was used successfully to : ( i ) reproduce the proton charge form ...**factor**1 - y ( b ) . Hence , the probability that the particle gets removed from the incident beam is 1— | 1 — y ( b ) ... Page 22

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**factors**make Coulomb corrections insignificant in do DT / do . How important are the details of the target nucleus wave function ? Not very important . The most important are general characteristics : density distributions ( hence ... Page 23

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**factor**to M = ( M ( △ ; 81 ... SA ) ) assuming the wave function to be in the form of a product of the c.m. wave function and the internal wave function . M = ( R ( r ) | exp ( i △ ⋅r ) | R ( r ) ) ( Þ 。( rı ′ . . . ra ′ ) | M ′ | Þ ... Page 24

Wiesław Czyż. Hence if we can

Wiesław Czyż. Hence if we can

**factor**out the c.m. wave function from the product = II ; ; ( r ; ) we can stick to calculating M with Yo but we have to multiply it by a correction**factor**: ( R ( r ) | exp ( i △ · r ) | R ( r ) ) −1 ... Page 25

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**factor**exp ( R242 / 4A ) . For small A ( say A = 2 , 3 or 4 ) it can be a correction of as much as 2 orders of magnitude for A2 0.3 GeV2 . A few concluding remarks about the deuteron target . A lot of attention was concentrated on 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