Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Results 1-5 of 5
Page 13
... EXCITED STATES Suppose we reject the intermediate excited states and take only the ground state as a possible inter- mediate state ( this is the way to eliminate all channels but one ) . Then each y ; can be averaged over r1 ( b ) ...
... EXCITED STATES Suppose we reject the intermediate excited states and take only the ground state as a possible inter- mediate state ( this is the way to eliminate all channels but one ) . Then each y ; can be averaged over r1 ( b ) ...
Page 14
... excited states , neither of ( b ) nor of ( a ) . So , the Chou & Yang [ 13 ] limit A , B → looses all excited state contributions and becomes ( 3.4 ) . Equation ( 3.4 ) gives the well - known " droplet model " [ 13 ] elastic scattering ...
... excited states , neither of ( b ) nor of ( a ) . So , the Chou & Yang [ 13 ] limit A , B → looses all excited state contributions and becomes ( 3.4 ) . Equation ( 3.4 ) gives the well - known " droplet model " [ 13 ] elastic scattering ...
Page 18
... excited states of the projectile present at intermediate steps ) are excluded . O O O They are the source of the so - called inelastic screening ( or inelastic shadowing ) phenomenon [ 47 ] . In order to include them we have to ascribe ...
... excited states of the projectile present at intermediate steps ) are excluded . O O O They are the source of the so - called inelastic screening ( or inelastic shadowing ) phenomenon [ 47 ] . In order to include them we have to ascribe ...
Page 62
... excited states . This makes good sense if one believes ( following Good and Walker [ 23 ] ) that in the high energy limit the ground and excited states of the incident system ( e.g. , a pion ) are considered to be approximately ...
... excited states . This makes good sense if one believes ( following Good and Walker [ 23 ] ) that in the high energy limit the ground and excited states of the incident system ( e.g. , a pion ) are considered to be approximately ...
Page 65
... excited states | m ) from which the system | 2 ) emerges . On the mass scale M ( mass ) m states < m | 5 | m > < mc1 weak transition the ground state which does not " mix " with m - states . Its elastic scattering profile is < 1 | r | 1 > ...
... excited states | m ) from which the system | 2 ) emerges . On the mass scale M ( mass ) m states < m | 5 | m > < mc1 weak transition the ground state which does not " mix " with m - states . Its elastic scattering profile is < 1 | r | 1 > ...
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 |