Interactions of High Energy Particles with Nuclei |
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To this end , the Bureau conducts research and provides : ( 1 ) a basis for the Nation's physical measurement system , ( 2 ) scientific and technological services for industry and government , ( 3 ) a technical basis for equity in trade ...
To this end , the Bureau conducts research and provides : ( 1 ) a basis for the Nation's physical measurement system , ( 2 ) scientific and technological services for industry and government , ( 3 ) a technical basis for equity in trade ...
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( c ) One may also hope that , in the cases where the scattering from a nucleus cannot be reduced to the " elementary amplitudes " of the incident particle - target nucleon , some new physical situa- tions may occur which stem from the ...
( c ) One may also hope that , in the cases where the scattering from a nucleus cannot be reduced to the " elementary amplitudes " of the incident particle - target nucleon , some new physical situa- tions may occur which stem from the ...
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We can also see that the physical reason for this phenomenon is the coupling between different spin states produced by the term K ( 81.B1 - id1 E102 ) . So , we have to deal with a coupled channels problem .
We can also see that the physical reason for this phenomenon is the coupling between different spin states produced by the term K ( 81.B1 - id1 E102 ) . So , we have to deal with a coupled channels problem .
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First we introduce the physical states of the system , | X ; ) ( which are analogous to the states „ and nye , of the photon ) . We want to compute ( X ; | TX ; ) . We expand | X ; ) into a set of states | A ) whose scattering and ...
First we introduce the physical states of the system , | X ; ) ( which are analogous to the states „ and nye , of the photon ) . We want to compute ( X ; | TX ; ) . We expand | X ; ) into a set of states | A ) whose scattering and ...
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[ S4 ] ) we express the states of the physical proton and the physical neutron - pion pair through the " bare " states of the proton ( p ) and the neutron - pion pair ( ññ ) . π Initial state : p = + = = d1o | μ ) + d1⁄23 | ññ ) p ñ ...
[ S4 ] ) we express the states of the physical proton and the physical neutron - pion pair through the " bare " states of the proton ( p ) and the neutron - pion pair ( ññ ) . π Initial state : p = + = = d1o | μ ) + d1⁄23 | ññ ) p ñ ...
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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 |