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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