Proceedings of the International School of Physics "Enrico Fermi.", Volume 11N. Zanichelli, 1960 - Nuclear physics |
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Page 303
1 ) leads to the usual V - A interaction form for this process , where gu = ta is the
coupling constant normally quoted . To account for the processes of nuclear B -
decay and of de capture by nuclei , a nucleon current term ( 1 . 3 ) jot = f ( n ya ( 1
+ ...
1 ) leads to the usual V - A interaction form for this process , where gu = ta is the
coupling constant normally quoted . To account for the processes of nuclear B -
decay and of de capture by nuclei , a nucleon current term ( 1 . 3 ) jot = f ( n ya ( 1
+ ...
Page 305
decay processes can arise through the interactions ( 1 . 1 ) which include the
factor J + 1 ) . The particular advantage of the interaction current hypothesis here
is that it excludes various type of interaction which do not appear to be present ,
for ...
decay processes can arise through the interactions ( 1 . 1 ) which include the
factor J + 1 ) . The particular advantage of the interaction current hypothesis here
is that it excludes various type of interaction which do not appear to be present ,
for ...
Page 310
However , for the interaction given by ( 2 . 5 ) , the only form allowed by the ( I ' , A
) theory , Sakurai ' s formula shows that this component of transverse polarization
is always zero , irrespective of the relative phase between Ck and BR , that is ...
However , for the interaction given by ( 2 . 5 ) , the only form allowed by the ( I ' , A
) theory , Sakurai ' s formula shows that this component of transverse polarization
is always zero , irrespective of the relative phase between Ck and BR , that is ...
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Contents
GENERALITÀ | 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