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

### From inside the book

Results 6-10 of 14

Page 45

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**measuring**σr ( y , nucleon ) one can determine ( do / d ) ( yp → pp ) |。 for which one gets much too high a value . One may get agreement if one reduces Y2 / 4 from 0.62 to 0.37 ! But y , 2 / 4π is well known from colliding beam ... Page 50

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**measurement**" is possible because the vector mesons interact with nucleons before they decay . The differential photoproduction cross sections look very much like elastic hadron - nucleus cross sections . They exhibit a steep slope at ... Page 51

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**measured**looks as follows : double scattering contributions do ( mb Gev2 ) 10 SINGLE SCATTERING D COMPONENT OF THE ...**measuring**the amplitudes for photoproduction of po on neutrons and protons , modulated by the deuteron form factor F ... Page 52

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**measuring**the cross section at large momentum transfers we can extract fnucleon because we know fynucleon quite well ...**measurement**of the elastic p - nucleon cross section in existence . ( ii ) If one wants to extract on or y , 2 / 4π ... Page 53

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**measured**was Y + A → po + A _ +++ 00 The following targets were used : H2 , Be , C , Al , Ti , Cu , Ag , Cd , In , Ta , W , Au , Pb , U. The parameters obtained from fitting the differential cross sections to their very extensive ...### 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