Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 13
... contribution of the second order because [ d3r , ®po® • ( r , ® ) ¥ u ( b − s , ® + 81® ) ) 2ı ( b − 8 , +82 ) ) % ( rz ) = = ( b ) [ dar , ®d3r , ®'ço © ® * ( ri ) vu ( b − 8 ; ® + si® ) Σ ¢ „ ® ( r¿® ) ¢ „ 6 ) * ( rzb ) ' ) XY21 ...
... contribution of the second order because [ d3r , ®po® • ( r , ® ) ¥ u ( b − s , ® + 81® ) ) 2ı ( b − 8 , +82 ) ) % ( rz ) = = ( b ) [ dar , ®d3r , ®'ço © ® * ( ri ) vu ( b − 8 ; ® + si® ) Σ ¢ „ ® ( r¿® ) ¢ „ 6 ) * ( rzb ) ' ) XY21 ...
Page 14
... contributions and becomes ( 3.4 ) . Equation ( 3.4 ) gives the well - known " droplet model " [ 13 ] elastic scattering amplitude of two composite objects whose hadronic matter distributions are given by pa ) ( s ( a ) ) and p ( b ) ( s ...
... contributions and becomes ( 3.4 ) . Equation ( 3.4 ) gives the well - known " droplet model " [ 13 ] elastic scattering amplitude of two composite objects whose hadronic matter distributions are given by pa ) ( s ( a ) ) and p ( b ) ( s ...
Page 16
... 1- ( r ) 2 gives the probability ( at the impact parameter b ) of losing the incident particle from the elastic channel . It is convenient however to split the second term into two physically different contributions : 16.
... 1- ( r ) 2 gives the probability ( at the impact parameter b ) of losing the incident particle from the elastic channel . It is convenient however to split the second term into two physically different contributions : 16.
Page 17
Wiesław Czyż. split the second term into two physically different contributions : [ ď2b [ 2 Re ( r ) − | ( r ) | 2 ] = [ ď3b [ ( r + r ) — | ( r ) | 2 ] = σDT + [ db [ 2 Re ( r ) — ( r + r ) ] = σ PROD Interpretation The first contribution ...
Wiesław Czyż. split the second term into two physically different contributions : [ ď2b [ 2 Re ( r ) − | ( r ) | 2 ] = [ ď3b [ ( r + r ) — | ( r ) | 2 ] = σDT + [ db [ 2 Re ( r ) — ( r + r ) ] = σ PROD Interpretation The first contribution ...
Page 18
... contributions to aror discussed above do approximately exhaust the list of processes contributing to elastic scattering . From our discussion of the components of σTOT ( σel , σDT , σPROD ) it follows that the measure- ments of σror may ...
... contributions to aror discussed above do approximately exhaust the list of processes contributing to elastic scattering . From our discussion of the components of σTOT ( σel , σDT , σPROD ) it follows that the measure- ments of σror may ...
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
Bibliographic information
| Title | Interactions of High Energy Particles with Nuclei Volume 139 of NBS monograph |
| Author | Wiesław Czyż |
| Publisher | National Bureau of Standards, 1975 |
| Original from | the University of Michigan |
| Digitized | 21 Nov 2007 |
| Length | 69 pages |
| Export Citation | BiBTeX EndNote RefMan |