Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 9
... mass of the particle . Note that eq ( 2.6 ) gives the same relation between magnetic moment and spin when x = 1 ! So , in both Examples , when к and ĩ are chosen to make eq ( 2.7 ) valid , the spin states decouple in the high energy ...
... mass of the particle . Note that eq ( 2.6 ) gives the same relation between magnetic moment and spin when x = 1 ! So , in both Examples , when к and ĩ are chosen to make eq ( 2.7 ) valid , the spin states decouple in the high energy ...
Page 23
... mass . Take , for example , a deuteron : here taking into account the c.m. motion is trivially accom- plished by using the wave functions of the relative motion , ø ( r ) . + R For example , the elastic scattering amplitude is M ( A ) ...
... mass . Take , for example , a deuteron : here taking into account the c.m. motion is trivially accom- plished by using the wave functions of the relative motion , ø ( r ) . + R For example , the elastic scattering amplitude is M ( A ) ...
Page 31
... masses , and thus can be considered as a two component degenerate system . When left in empty space , however , both Ko and Ko , decay weakly with two different lifetimes as if they were made up of two different particles , which is ...
... masses , and thus can be considered as a two component degenerate system . When left in empty space , however , both Ko and Ko , decay weakly with two different lifetimes as if they were made up of two different particles , which is ...
Page 35
... masses differ . This fact may introduce some important corrections at low energies . But in the limit of very high energies and small momentum transfer , all such effects dis- appear . Let us take , e.g. , two such states and give them ...
... masses differ . This fact may introduce some important corrections at low energies . But in the limit of very high energies and small momentum transfer , all such effects dis- appear . Let us take , e.g. , two such states and give them ...
Page 41
... mass of the n- system : Mnr2 = ( √ẞ2w2 + p12 + mn2 + √ ( 1 − ẞ ) 2w2 + p12 + m , 2 ) 2 - ( p1 - p1 ) 2 - ( Bw + ( 1 − ẞ ) w ) 2 843 1 B ( 1-8 ) [ p12 + m , 2 ( 1 − ß ) + m‚2ß ] , and the four - momentum transfers : -tpm , 2 + B ...
... mass of the n- system : Mnr2 = ( √ẞ2w2 + p12 + mn2 + √ ( 1 − ẞ ) 2w2 + p12 + m , 2 ) 2 - ( p1 - p1 ) 2 - ( Bw + ( 1 − ẞ ) w ) 2 843 1 B ( 1-8 ) [ p12 + m , 2 ( 1 − ß ) + m‚2ß ] , and the four - momentum transfers : -tpm , 2 + B ...
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