Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Results 1-5 of 21
Page 3
... მ 22 hence , neglecting second derivatives of , we obtain the following equation for : 2ikeika = ду 2m Əz h2 Veiks , მო Əz = vh V❤ , where we have used Р p = kh , v = • m The amplitude for the particle to scatter from k to 3.
... მ 22 hence , neglecting second derivatives of , we obtain the following equation for : 2ikeika = ду 2m Əz h2 Veiks , მო Əz = vh V❤ , where we have used Р p = kh , v = • m The amplitude for the particle to scatter from k to 3.
Page 4
... obtaining the fundamental formula ( 2.1 ) ; the reliability of this formula is of primary importance . The most complete analysis one can perform is presumably to employ the Watson multiple scattering theory , but we shall not present ...
... obtaining the fundamental formula ( 2.1 ) ; the reliability of this formula is of primary importance . The most complete analysis one can perform is presumably to employ the Watson multiple scattering theory , but we shall not present ...
Page 11
... obtain 2ka2 = 2X10 GeVX25 GeV - 2 = 100 fm . Note that ( 3.1 ) gives , as r → ∞ , ( compare D. R. Yennie article in [ S3 ] ) ↓ ( r ) = eik z + [ ƒ ( ke ) / r ] exp ( ikr ) , ( e = component of re , ) , with f ( ke ) correctly given ...
... obtain 2ka2 = 2X10 GeVX25 GeV - 2 = 100 fm . Note that ( 3.1 ) gives , as r → ∞ , ( compare D. R. Yennie article in [ S3 ] ) ↓ ( r ) = eik z + [ ƒ ( ke ) / r ] exp ( ikr ) , ( e = component of re , ) , with f ( ke ) correctly given ...
Page 21
... obtained by integrating p ( r ) over z . The parameters of x . ( b ) were taken from proton - nucleon scat- tering cross sections . For an αp = −0.33 , σn = op = 38.9 mb ( these parameters are resonable for ~ 20 GeV protons ) , one ...
... obtained by integrating p ( r ) over z . The parameters of x . ( b ) were taken from proton - nucleon scat- tering cross sections . For an αp = −0.33 , σn = op = 38.9 mb ( these parameters are resonable for ~ 20 GeV protons ) , one ...
Page 30
... obtained the result completely analogous to the one obtained for the optical diffractive production : for i # j the production amplitude is proportional to the difference in absorptions of the i , j components . This is a very general ...
... obtained the result completely analogous to the one obtained for the optical diffractive production : for i # j the production amplitude is proportional to the difference in absorptions of the i , j components . This is a very general ...
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