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 analysis approximately assume attenuation beam coherent collision complete components compute consider contribution corrections Coulomb Coulomb interactions coupling cross section db exp db exp i▲·b depend describe deuteron diffractive production processes discussed effects elastic scattering elastic scattering amplitude equation example excited existence experimental experiments expression fact factor field final formula forward given gives Glauber ground hadrons Hence high energy limit important incident particle inelastic initial Institute interactions introduce magnetic mass measurement momentum transfer multiple scattering Note nuclear nuclear targets nuclei nucleon numbers objects obtained parameters phase shifts photon photoproduction physical position possible problem profiles regeneration shadowing single Standards step strong structure technical vector meson wave function weak