Proceedings of the International School of Physics "Enrico Fermi.", Volume 11N. Zanichelli, 1960 - Nuclear physics |
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Page 236
In J J transitions , on the other hand , both types of interaction will in general
contribute both « pure » » ( r = . ... We may accordingly speak in a general way of
« pure Fermi » , « pure Gamow Teller » ) and « mixed » contributions to the
double ...
In J J transitions , on the other hand , both types of interaction will in general
contribute both « pure » » ( r = . ... We may accordingly speak in a general way of
« pure Fermi » , « pure Gamow Teller » ) and « mixed » contributions to the
double ...
Page 307
However the set of intermediate baryon - pair states which contribute to Kit decay
is different from that which contributes to Torta decay ; it is also possible that the K
- meson parity ( relative to that for the A hyperon ) may not be the same as the ...
However the set of intermediate baryon - pair states which contribute to Kit decay
is different from that which contributes to Torta decay ; it is also possible that the K
- meson parity ( relative to that for the A hyperon ) may not be the same as the ...
Page 357
11 ) does not contribute to the matrix element ; the last two terms can be shown to
give contributions which can be thought of as included in the subtraction constant
of the dispersion relations ; the second term has the right form of an advanced ...
11 ) does not contribute to the matrix element ; the last two terms can be shown to
give contributions which can be thought of as included in the subtraction constant
of the dispersion relations ; the second term has the right form of an advanced ...
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Contents
GENERALITĄ | 1 |
PARTE PRIMA Problemi teorici | 9 |
PARTE SECONDA Correlazioni angolari polarizzazioni e decadimenti beta | 197 |
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allowed angle angular assumed calculated charge classical combination completely component connection conservation consider constant contribute correlation corresponding coupling curvature decay defined density dependence derived described determination direction discussed effects electric electromagnetic field electron element elementary emission energy equations example existence experiment experimental expression factor Fermi field final finds formula function geometrodynamics geometry give given gravitational histories initial interaction invariance known leads limit magnetic mass matrix means measured metric modes momentum neutrino neutron nuclei nucleons observed obtained operators pairs parity particle phase Phys physics polarization possible present principle problem properties purely quantity quantum quantum mechanics question radiation ratio reason reference relation relativity requires respect result scattering shown shows solution space spin symmetry Table theory transformation transitions universe vector wave weak zero