Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Page 13
... nucleons are " equivalent " ) đ3b exp ( i △ · b ) [ d23⁄4 ̧ @ ...... ď23⁄4 ̧ @ Ĥp ́ ( 8 , ̧ • ) { 1− ĤI ( 1−5μ ( b + 8 , ̧ ° ) ) " }。( a ) đỏ exp ( iA + b ) ( d8 ... 81 · { 1– ÎI ( 1 – Ã ‚ ( b + s , ( ... ) ) } ÎI ¿ ̈ ) ...
... nucleons are " equivalent " ) đ3b exp ( i △ · b ) [ d23⁄4 ̧ @ ...... ď23⁄4 ̧ @ Ĥp ́ ( 8 , ̧ • ) { 1− ĤI ( 1−5μ ( b + 8 , ̧ ° ) ) " }。( a ) đỏ exp ( iA + b ) ( d8 ... 81 · { 1– ÎI ( 1 – Ã ‚ ( b + s , ( ... ) ) } ÎI ¿ ̈ ) ...
Page 14
... nucleon phase shifts . But that means that this additivity improves with increase of the binding of ( b ) . Of course for R - 0 the additivity becomes exact . One can see this explicitly by replacing for ( b ) , pb ) ( s ) ~ ( 2 ) ( s ) ...
... nucleon phase shifts . But that means that this additivity improves with increase of the binding of ( b ) . Of course for R - 0 the additivity becomes exact . One can see this explicitly by replacing for ( b ) , pb ) ( s ) ~ ( 2 ) ( s ) ...
Page 17
... nucleons of the target nucleus : σ PROD = < / d2b [ 1-113 ] ) = d26 [ 1- ( 1 − r | 3 ) ] √ = [ d3b [ 2 Re ( r ) ... nucleons frozen at the positions $ 1 , SA . .. • So , in our model there are three different contributions . OEL ONLY ...
... nucleons of the target nucleus : σ PROD = < / d2b [ 1-113 ] ) = d26 [ 1- ( 1 − r | 3 ) ] √ = [ d3b [ 2 Re ( r ) ... nucleons frozen at the positions $ 1 , SA . .. • So , in our model there are three different contributions . OEL ONLY ...
Page 21
... nucleon scat- tering cross sections . For an ap = -0.33 , σn = 0 , = 38.9 mb ( these parameters are resonable for ... nucleons . ( b / sr ) d & LAB 10 103 10 O 100 % 10 5 10 NEUTRAL NEGATIVE CHARGE POSITIVE CHARGE 15 20 PLAB , mrad For ...
... nucleon scat- tering cross sections . For an ap = -0.33 , σn = 0 , = 38.9 mb ( these parameters are resonable for ... nucleons . ( b / sr ) d & LAB 10 103 10 O 100 % 10 5 10 NEUTRAL NEGATIVE CHARGE POSITIVE CHARGE 15 20 PLAB , mrad For ...
Page 22
... nucleons " is a A · [ d3b p ( b ) e ̄ • Ap ‹ b ) , where σ is an average total hadron - nucleon cross section . If indeed σDT / dî has such a form , the only place where Coulomb interactions enter are in the individual proton amplitudes ...
... nucleons " is a A · [ d3b p ( b ) e ̄ • Ap ‹ b ) , where σ is an average total hadron - nucleon cross section . If indeed σDT / dî has such a form , the only place where Coulomb interactions enter are in the individual proton amplitudes ...
Common terms and phrases
absorption additivity of phase anomalous magnetic moment ú approximately assume attenuation b+½s beam Bureau of Standards coherent diffractive production collision Compton scattering compute Coulomb interactions Czyż d³r 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 γν Σ Σ