Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 14
... deuteron - deuteron scattering data are available , but reliable calculations are very difficult because of the high spins involved . Nevertheless , there exist some calculations [ S1 ] and there seems to be reasonable agreement between ...
... deuteron - deuteron scattering data are available , but reliable calculations are very difficult because of the high spins involved . Nevertheless , there exist some calculations [ S1 ] and there seems to be reasonable agreement between ...
Page 23
... 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 ) = ik 2π db exp ( i △ · b ) ƒ ...
... 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 ) = ik 2π db exp ( i △ · b ) ƒ ...
Page 25
... deuteron target . A lot of attention was concentrated on the deuteron because it is a very important testing ground for multiple scattering theories ( or models ) . ( i ) In experiments ( compare deuteron data contained in [ S1 ] ...
... deuteron target . A lot of attention was concentrated on the deuteron because it is a very important testing ground for multiple scattering theories ( or models ) . ( i ) In experiments ( compare deuteron data contained in [ S1 ] ...
Page 26
... deuteron ground state ) . Let us discuss this effect in more detail . The ground state deuteron wave function is : Pm ( r ) = ( 4π ) -1 / 2-1 [ u ( r ) + 8-1 / 2 S12W ( r ) Jx1.m where u ( r ) and w ( r ) are the radial S and D ...
... deuteron ground state ) . Let us discuss this effect in more detail . The ground state deuteron wave function is : Pm ( r ) = ( 4π ) -1 / 2-1 [ u ( r ) + 8-1 / 2 S12W ( r ) Jx1.m where u ( r ) and w ( r ) are the radial S and D ...
Page 27
... deuteron example . In the standard Glauber model , it is enough to have p ( s ) = √∞ dzó 。* ( s , z ) Þo ( s , z ) to compute the cross section . Suppose there is some deformation in the final state : Po * ( s , 2 ) → o ' * ( A , s ...
... deuteron example . In the standard Glauber model , it is enough to have p ( s ) = √∞ dzó 。* ( s , z ) Þo ( s , z ) to compute the cross section . Suppose there is some deformation in the final state : Po * ( s , 2 ) → o ' * ( A , s ...
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 |
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