Interactions of High Energy Particles with Nuclei |
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Page 32
... Ko interact differently with matter , they are absorbed differently . ( e.g. , K ° ( S = -1 ) + p — 4 ° ( S = -1 ) +7+ while Ko ( S = + 1 ) cannot produce Ao ) . In figure 18 the so - called transmission regeneration is sketched .
... Ko interact differently with matter , they are absorbed differently . ( e.g. , K ° ( S = -1 ) + p — 4 ° ( S = -1 ) +7+ while Ko ( S = + 1 ) cannot produce Ao ) . In figure 18 the so - called transmission regeneration is sketched .
Page 34
... frop -3 for ~ 4 GeV / c 2 Ref ( in fermis ) -1 +1 From this picture it is clear that neutrons are much more effective in regeneration than protons ( the difference in absorption of K and Ko is much bigger in the case of neutrons ) .
... frop -3 for ~ 4 GeV / c 2 Ref ( in fermis ) -1 +1 From this picture it is clear that neutrons are much more effective in regeneration than protons ( the difference in absorption of K and Ko is much bigger in the case of neutrons ) .
Page 43
... where the photon is absorbed by the target ( or part of it ) and re - emitted . E.g. , when the total Compton amplitude is a sum of individual ( photon - nucleon ) Compton amplitudes MCOMPTON ( q ) = exp ( iq.r ; ) MCO MPTON ( ) ( a ) ...
... where the photon is absorbed by the target ( or part of it ) and re - emitted . E.g. , when the total Compton amplitude is a sum of individual ( photon - nucleon ) Compton amplitudes MCOMPTON ( q ) = exp ( iq.r ; ) MCO MPTON ( ) ( a ) ...
Page 58
Discussion of the Anomalously Small Absorption of 37 and 51 Systems in Nuclear Matter First , let us stress that there is no satisfactory explanation of this phenomenon available . One can , nevertheless , make a few points which may ...
Discussion of the Anomalously Small Absorption of 37 and 51 Systems in Nuclear Matter First , let us stress that there is no satisfactory explanation of this phenomenon available . One can , nevertheless , make a few points which may ...
Page 61
Perhaps at this stage one should point out that one could easily explain the small absorption cross section by abandoning the “ one step ” description . The price to pay for it would be the loss of the interpretation of the states 1 ...
Perhaps at this stage one should point out that one could easily explain the small absorption cross section by abandoning the “ one step ” description . The price to pay for it would be the loss of the interpretation of the states 1 ...
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