Interactions of High Energy Particles with Nuclei |
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Page 14
To the best of my knowledge , only 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 the best of my knowledge , only 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 ...
Page 23
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 ) = ik 2π ...
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 ) = ik 2π ...
Page 25
A few concluding remarks about the 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 ...
A few concluding remarks about the 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 ...
Page 26
( ii ) One can also see ( again , compare [ S1 ] ) how important the deformation of the target is ( existence of the D - state in the deuteron ground state ) . Let us discuss this effect in more detail . The ground state deuteron wave ...
( ii ) One can also see ( again , compare [ S1 ] ) how important the deformation of the target is ( existence of the D - state in the deuteron ground state ) . Let us discuss this effect in more detail . The ground state deuteron wave ...
Page 27
Incidentally , only the spin of the deuteron as a whole is essential . The qualitative effect is independent of the spin of the incident particle ( the M ( △ , s ) operator does not act on spin quantum numbers . ) ...
Incidentally , only the spin of the deuteron as a whole is essential . The qualitative effect is independent of the spin of the incident particle ( the M ( △ , s ) operator does not act on spin quantum numbers . ) ...
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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 |