Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Results 1-5 of 15
Page 1
... beams ) . Nevertheless , one still hopes to be able to learn something new , for example about short range nucleon correlation functions in target nuclei or about the pres- ence of resonances in nuclear ground states [ 3 , 4 ] -just to ...
... beams ) . Nevertheless , one still hopes to be able to learn something new , for example about short range nucleon correlation functions in target nuclei or about the pres- ence of resonances in nuclear ground states [ 3 , 4 ] -just to ...
Page 15
... gets removed from the incident beam is 1— | 1 — y ( b ) | 2 = 2 Rey ( b ) ( b ) 2 ( at the impact parameter b ) . Notice that here we use the same expression as in the following paragraphs : we identify 1–7 with y 15.
... gets removed from the incident beam is 1— | 1 — y ( b ) | 2 = 2 Rey ( b ) ( b ) 2 ( at the impact parameter b ) . Notice that here we use the same expression as in the following paragraphs : we identify 1–7 with y 15.
Page 19
... beam of particles . For isospin zero targets ( He , 160 ) , if one finds no difference between the elastic cross section for and it implies that there is no real part in the π - nucleus elastic scattering strong interaction phase shift ...
... beam of particles . For isospin zero targets ( He , 160 ) , if one finds no difference between the elastic cross section for and it implies that there is no real part in the π - nucleus elastic scattering strong interaction phase shift ...
Page 22
... beam ( ~ 50 MeV ) , hence they sum over all 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 ) ...
... beam ( ~ 50 MeV ) , hence they sum over all 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 ) ...
Page 31
... beam and its scattering ( elastic ) properties are known reasonably well . The trouble is with the outgoing objects ; e.g. , when 3 are produced in the → 3 reaction : are then its n's given by the absorption of 37 in the target ? In ...
... beam and its scattering ( elastic ) properties are known reasonably well . The trouble is with the outgoing objects ; e.g. , when 3 are produced in the → 3 reaction : are then its n's given by the absorption of 37 in the target ? In ...
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