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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... 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 situations may occur which stem from the complexity of the target .
... 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 situations may occur which stem from the complexity of the target .
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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 ( 01.B. - id..E10 ) . So , we have to deal with a coupled channels problem . We can make the following ...
We can also see that the physical reason for this phenomenon is the coupling between different spin states produced by the term K ( 01.B. - id..E10 ) . So , we have to deal with a coupled channels problem . We can make the following ...
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... 1-11- ( T ) | 2 gives the probability ( at the impact parameter b ) of losing the incident particle from the elastic channel . It is convenient however to split the second term into two physically different contributions : 16.
... 1-11- ( T ) | 2 gives the probability ( at the impact parameter b ) of losing the incident particle from the elastic channel . It is convenient however to split the second term into two physically different contributions : 16.
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split the second term into two physically different contributions : | < b [ 2 Re ( r ) – [ { r } / # ] = [ [ < r + r ) – 1 ( T ) | : ] = ODT + | dob [ 2 Re ( T ) – ( + r ) ] = O PROD = Interpretation The first contribution ( opt ) comes ...
split the second term into two physically different contributions : | < b [ 2 Re ( r ) – [ { r } / # ] = [ [ < r + r ) – 1 ( T ) | : ] = ODT + | dob [ 2 Re ( T ) – ( + r ) ] = O PROD = Interpretation The first contribution ( opt ) comes ...
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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 |