Interactions of High Energy Particles with Nuclei |
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Page 9
It is enough to observe that in Example 1 for k = 0 , the relation between the magnetic moment M and spin S is = les M ( 2.7 ) m where e is the charge and m the mass of the particle . Note that eq ( 2.6 ) gives the same relation between ...
It is enough to observe that in Example 1 for k = 0 , the relation between the magnetic moment M and spin S is = les M ( 2.7 ) m where e is the charge and m the mass of the particle . Note that eq ( 2.6 ) gives the same relation between ...
Page 23
When we want to discuss light nuclei we have to consider carefully the motion of the center of mass . Take , for example , a deuteron : here taking into account the c.m. motion is trivially accomplished by using the wave functions of ...
When we want to discuss light nuclei we have to consider carefully the motion of the center of mass . Take , for example , a deuteron : here taking into account the c.m. motion is trivially accomplished by using the wave functions of ...
Page 31
which have the same masses , and thus can be considered as a two component degenerate system . When left in empty space , however , both Ko and K , decay weakly with two different lifetimes as if they were made up of two different ...
which have the same masses , and thus can be considered as a two component degenerate system . When left in empty space , however , both Ko and K , decay weakly with two different lifetimes as if they were made up of two different ...
Page 35
Generalizing to Other Diffractive Production ( and Excitation ) Processes First of all , the components of the incident and the produced states are , in general , not degenerate : their invariant masses differ . This fact may introduce ...
Generalizing to Other Diffractive Production ( and Excitation ) Processes First of all , the components of the incident and the produced states are , in general , not degenerate : their invariant masses differ . This fact may introduce ...
Page 41
One can compute similarly the invariant mass of the n - system : Mnr * ' = ( VB ? w2 + p + + mn ? + V ( 1 - B ) ? w + p ?? + m72 ) 2- ( pı - p + ) 2- ( Bw + ( 1 - B ) w ) ? 1 [ p_a + m ,? ( 1-1 ) + m728 ] , B ( 1 - B ) and the four ...
One can compute similarly the invariant mass of the n - system : Mnr * ' = ( VB ? w2 + p + + mn ? + V ( 1 - B ) ? w + p ?? + m72 ) 2- ( pı - p + ) 2- ( Bw + ( 1 - B ) w ) ? 1 [ p_a + m ,? ( 1-1 ) + m728 ] , B ( 1 - B ) and the four ...
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absorption additivity analysis approximately assume attenuation beam Bureau of Standards charge coherent collision complete components compute consider contribution corrections Coulomb Coulomb interactions coupling cross section db exp depend describe deuteron diffractive production processes discussed effects elastic scattering elastic scattering amplitude equation example excited existence exp ia.b 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 National Bureau Note nuclear nuclear targets nuclei nucleon numbers objects obtained parameters phase shifts photon photoproduction physical position possible present problem profiles regeneration shadowing single Standards step strong structure technical vector meson wave function
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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