Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Results 6-10 of 26
Page 21
... nuclear boundary sin ( x . ( b ) + § ( b ) ) is large . It is amusing that numerically Im M with proper x . is approximately the same as Re M without xe ! This is true for 208 Pb . In general one gets all kinds of intermediate ...
... nuclear boundary sin ( x . ( b ) + § ( b ) ) is large . It is amusing that numerically Im M with proper x . is approximately the same as Re M without xe ! This is true for 208 Pb . In general one gets all kinds of intermediate ...
Page 22
... nuclear excitations ( without producing mesons , however ) . The cross section for such " inclusive " processes is do sc ΦΩ = n n ik Σ db exp ( i △ · b ) ( Y2 | Ã ( b ; 81 . . . 8. ) | Yo ) 12 = ( 2π ) 2 2π d2b d2b ′ exp [ i △ · ( b ...
... nuclear excitations ( without producing mesons , however ) . The cross section for such " inclusive " processes is do sc ΦΩ = n n ik Σ db exp ( i △ · b ) ( Y2 | Ã ( b ; 81 . . . 8. ) | Yo ) 12 = ( 2π ) 2 2π d2b d2b ′ exp [ i △ · ( b ...
Page 28
... nuclear targets supplement each other because the nuclear medium amplifies the scattering of the produced objects . The model of diffractive processes described below is based on : M. L. Good and W. D. Walker ( 1960 ) [ 23 ] . The ...
... nuclear targets supplement each other because the nuclear medium amplifies the scattering of the produced objects . The model of diffractive processes described below is based on : M. L. Good and W. D. Walker ( 1960 ) [ 23 ] . The ...
Page 33
... rather poor . The real and imaginary parts of the elastic Ko and Ão — nuclear amplitudes are sketched below . The uncertainties of our knowledge of these amplitudes are also shown [ 26 ] . 3 Imf ( in fermis ) ** P for ~ 333.
... rather poor . The real and imaginary parts of the elastic Ko and Ão — nuclear amplitudes are sketched below . The uncertainties of our knowledge of these amplitudes are also shown [ 26 ] . 3 Imf ( in fermis ) ** P for ~ 333.
Page 34
... nuclear 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 ...
... nuclear 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 ...
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