Proceedings of the International School of Physics "Enrico Fermi.", Volume 11N. Zanichelli, 1960 - Nuclear physics |
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Page 33
Consequences of Invariance under Parity and under Charge Conjugation . 1 . -
Eigenvalues . In contrast to the operator of time reversal the operators of parity
and charge conjugation are linear and unitary and , therefore , possess ...
Consequences of Invariance under Parity and under Charge Conjugation . 1 . -
Eigenvalues . In contrast to the operator of time reversal the operators of parity
and charge conjugation are linear and unitary and , therefore , possess ...
Page 34
For the intrinsic parity we find ( IV . 7 ) PY , + = in . Ve + and for that of the
antiparticle ( IV . 8 ) P„ ; - = inn - . Though we did not make that clear in the
notations the ne in general differ from field to field . For the standard form eqs . (
11 . 36 ) , ( II .
For the intrinsic parity we find ( IV . 7 ) PY , + = in . Ve + and for that of the
antiparticle ( IV . 8 ) P„ ; - = inn - . Though we did not make that clear in the
notations the ne in general differ from field to field . For the standard form eqs . (
11 . 36 ) , ( II .
Page 35
Only the intrinsic parity of strictly neutral bosons ( i . e . of the neutral 7° mesong )
is defined absolutely ( empirically it is odd ) . The generalized charges one has to
consider in connection with the ambiguities are those which are conserved in ...
Only the intrinsic parity of strictly neutral bosons ( i . e . of the neutral 7° mesong )
is defined absolutely ( empirically it is odd ) . The generalized charges one has to
consider in connection with the ambiguities are those which are conserved in ...
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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