Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Results 6-10 of 15
Page 21
... parameters of x . ( b ) were taken from proton - nucleon scat- tering cross sections . For an ap = -0.33 , σn = 0 , = 38.9 mb ( these parameters are resonable for ~ 20 GeV protons ) , one gets the following table = xc ( b ) + ( b ) ...
... parameters of x . ( b ) were taken from proton - nucleon scat- tering cross sections . For an ap = -0.33 , σn = 0 , = 38.9 mb ( these parameters are resonable for ~ 20 GeV protons ) , one gets the following table = xc ( b ) + ( b ) ...
Page 24
... parameter in the Gaussian factor in harmonic oscillator wave functions : exp ( -2 / 2R2 ) . Then ( R ( r ) | exp ( ¿ △ • r ) | ® ( r ) ) −1 = exp ( 42R2 / 4A ) . When one cannot do this factorization the computations become quite ...
... parameter in the Gaussian factor in harmonic oscillator wave functions : exp ( -2 / 2R2 ) . Then ( R ( r ) | exp ( ¿ △ • r ) | ® ( r ) ) −1 = exp ( 42R2 / 4A ) . When one cannot do this factorization the computations become quite ...
Page 31
... parameters n ; are determined by elastic scattering of real particles . The inelastic amplitude ( X ; | T | X ; ) = ( 1 — ni ) ei ; — ( 1 — nj ) E ij ( 4.4 ) is proportional to the difference between the absorption of the produced ...
... parameters n ; are determined by elastic scattering of real particles . The inelastic amplitude ( X ; | T | X ; ) = ( 1 — ni ) ei ; — ( 1 — nj ) E ij ( 4.4 ) is proportional to the difference between the absorption of the produced ...
Page 34
... parameters from the best fits [ 26 ] . Pb Cu ش تم Rp 6.60 fm 4.23 fm these are well known from 0.50 fm 0.57 fm Rn ( Cn = Cp ) Cn ( Rn = Rp ) ( 7.29 ± 0.13 ) fm ( 0.68 ± 0.04 ) fm elastic scat- tering ( 4.86 ± 0.10 ) fm ( 0.74 ± 0.03 ) ...
... parameters from the best fits [ 26 ] . Pb Cu ش تم Rp 6.60 fm 4.23 fm these are well known from 0.50 fm 0.57 fm Rn ( Cn = Cp ) Cn ( Rn = Rp ) ( 7.29 ± 0.13 ) fm ( 0.68 ± 0.04 ) fm elastic scat- tering ( 4.86 ± 0.10 ) fm ( 0.74 ± 0.03 ) ...
Page 40
... limit w∞ ( longitudinal component of the incident . momentum very large ) . There are two independent variables which may be chosen as pi , B. ( Here ẞ is an arbitrary parameter , 0 < ß < 1 ) . 1 = Ep - En - E , 843 1 40.
... limit w∞ ( longitudinal component of the incident . momentum very large ) . There are two independent variables which may be chosen as pi , B. ( Here ẞ is an arbitrary parameter , 0 < ß < 1 ) . 1 = Ep - En - E , 843 1 40.
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