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

### From inside the book

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**ground**states [ 3 , 4 ] —just to name two problems . ( c ) One may also hope that , in the cases where the scattering from a nucleus cannot be reduced to the " elementary amplitudes " of the incident particle - target nucleon , some new ... Page 12

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**ground**state wave functions are : B ¥ ‹ a ) = ÏÏ 40 ( r ; ( a ) ) , ¥ ( b ) = II 40 ( r¿ ( b ) ) , j Z and the elastic scattering amplitude is , therefore : M = ik 2π db exp ( i △ · b ) fď3r® ) ... .. d3r ̧ ‹ ° ) d3r , ∞ ) ( a ) I ... Page 13

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**ground**state as a possible inter- mediate state ( this is the way to eliminate all channels but one ) . Then each y , can be averaged over r¿ ‹ 3 ) : [ ď3r , b ) | ¢ o® ) ( r , b ) | 2 1 ; 1 ( b − s , 6 ) + s , ( « ) ) = [ d's , ®p ... Page 22

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**ground**state ) . In order to have a genuine elastic scattering one would have to have an energy resolution AE a fraction of an MeV , which for E ~ 20 GeV is still inaccessible . Most experiments ( e.g. , CERN series - compare [ S1 ] ... Page 24

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**ground**state wave function is a Gaussian [ 19 ] . The**ground**state densities and the elementary amplitudes are taken in the form Yo | 2 = ÎI p ( r ; ) , Ĥp f ( k ) = j = 1 ( i + a ) ko Απ p ( r ) = p 。 exp ( −r , 2 / R2 ) exp ...### Common terms and phrases

absorption additivity of phase anomalous magnetic moment Ãº approximately assume attenuation beam Bureau of Standards coherent diffractive production collision Compton scattering compute Coulomb interactions Czyż d³r db bJo db exp i▲·b deuteron diagonalization diffractive production processes diffractive scattering discussed double scattering elastic scattering amplitude electromagnetic equation example excited experiments factor Feynman diagrams formula four-momentum Glauber model hadrons Hence high energy limit incident particle incident wave inelastic shadowing Interactions of High invariant mass K mesons multiple scattering National Bureau neutrino neutrons ññ Note nuclear matter nuclear targets nuclei nucleon obtained optical theorem parameters phase shifts photon photoproduction of vector physical pion production amplitude profiles quantum numbers regeneration Řº shadowing effects single scattering spin strongly interacting target nucleus total cross section vector meson VMD model wave function Απ γν ΦΩ