Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Results 1-5 of 8
Page 2
... momentum of the incident particle in laboratory frame A is the two - dimensional momentum transfer b is the impact parameter x ; ( b ) is the phase shift which characterizes the incident particle - jth nucleon elastic scat- tering ...
... momentum of the incident particle in laboratory frame A is the two - dimensional momentum transfer b is the impact parameter x ; ( b ) is the phase shift which characterizes the incident particle - jth nucleon elastic scat- tering ...
Page 11
... momentum transfer is d≈a1 . We can then estimate the " healing " length , L , of the shadow : L 1 , L < 2ka2 ; 2ka2 for a = 1 fm , k = 10 GeV we obtain 2ka2 = 2X10 GeVX25 GeV - 2 = 100 fm . Note that ( 3.1 ) gives , as r ...
... momentum transfer is d≈a1 . We can then estimate the " healing " length , L , of the shadow : L 1 , L < 2ka2 ; 2ka2 for a = 1 fm , k = 10 GeV we obtain 2ka2 = 2X10 GeVX25 GeV - 2 = 100 fm . Note that ( 3.1 ) gives , as r ...
Page 27
... momentum transfer ( 42≈2 GeV2 ) . What is the cause ? Perhaps some relativistic effects ? There is no good answer , so far . Without going into any explanation of this discrepancy , let us em- phasize the following point : It is ...
... momentum transfer ( 42≈2 GeV2 ) . What is the cause ? Perhaps some relativistic effects ? There is no good answer , so far . Without going into any explanation of this discrepancy , let us em- phasize the following point : It is ...
Page 35
... momentum transfer can also be neglected . So , in the limit p → 0 all the states taking part in diffractive production processes can be considered degenerate and the longitudinal momentum transfer neglected . As was said , however ...
... momentum transfer can also be neglected . So , in the limit p → 0 all the states taking part in diffractive production processes can be considered degenerate and the longitudinal momentum transfer neglected . As was said , however ...
Page 43
... momentum transfer and r ; are position vectors of the nucleons in the target nucleus , it gives the following contribution to the total photon - nucleus cross section ( which is proportional to A ) : 4π Im MCOMPTON ( 0 ) = A k N or ( YP ) ...
... momentum transfer and r ; are position vectors of the nucleons in the target nucleus , it gives the following contribution to the total photon - nucleus cross section ( which is proportional to A ) : 4π Im MCOMPTON ( 0 ) = A k N or ( YP ) ...
Common terms and phrases
absorption additivity of phase anomalous magnetic moment ú 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