Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Results 6-10 of 14
Page 32
... absorbed differently . ( e.g. , Ko ( S = −1 ) + p → Ao ( S = − 1 ) + π + while K ° ( S = + 1 ) cannot produce Ao ) . In figure 18 the so - called transmission regeneration is sketched . ко ко MACROSCOPIC TARGET One can , however ...
... absorbed differently . ( e.g. , Ko ( S = −1 ) + p → Ao ( S = − 1 ) + π + while K ° ( S = + 1 ) cannot produce Ao ) . In figure 18 the so - called transmission regeneration is sketched . ко ко MACROSCOPIC TARGET One can , however ...
Page 34
... absorption of Ão and Ko is much bigger in the case of neutrons ) . One can get excellent fits to the differential cross sections doKL - Ks / dA2 by making the neutron and proton distributions different . One gets the following nuclear ...
... absorption of Ão and Ko is much bigger in the case of neutrons ) . One can get excellent fits to the differential cross sections doKL - Ks / dA2 by making the neutron and proton distributions different . One gets the following nuclear ...
Page 43
... absorbed by the target ( or part of it ) and re - emitted . E.g. , when the total Compton amplitude is a sum of individual ( photon - nucleon ) Compton amplitudes = Σ MCOMPTON ( 9 ) Σ exp ( iq⋅r ; ) MCOMPTON ( q ) where q is the three ...
... absorbed by the target ( or part of it ) and re - emitted . E.g. , when the total Compton amplitude is a sum of individual ( photon - nucleon ) Compton amplitudes = Σ MCOMPTON ( 9 ) Σ exp ( iq⋅r ; ) MCOMPTON ( q ) where q is the three ...
Page 58
... Absorption of 3 and 5π Systems in Nuclear Matter First , let us stress that there is no satisfactory explanation of this phenomenon available . One can , nevertheless , make a few points which may advance a bit our understanding of the ...
... Absorption of 3 and 5π Systems in Nuclear Matter First , let us stress that there is no satisfactory explanation of this phenomenon available . One can , nevertheless , make a few points which may advance a bit our understanding of the ...
Page 61
... absorption cross section by abandoning the " one step " description . The price to pay for it would be the loss of the interpretation of the states | I ) and | 2 ) as “ almost " a one physical pion state and “ almost " a three physical ...
... absorption cross section by abandoning the " one step " description . The price to pay for it would be the loss of the interpretation of the states | I ) and | 2 ) as “ almost " a one physical pion state and “ almost " a three physical ...
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