Proceedings of the International School of Physics "Enrico Fermi.", Volume 11N. Zanichelli, 1960 - Nuclear physics |
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Page 54
A simple calculation based on equation ( 54 ) shows for example that and pio
have the same significant part , namely pilo ) . ( For obvious reasons pi as well as
E count as antisymmetrical operators ! ) . Another interesting example is
presented ...
A simple calculation based on equation ( 54 ) shows for example that and pio
have the same significant part , namely pilo ) . ( For obvious reasons pi as well as
E count as antisymmetrical operators ! ) . Another interesting example is
presented ...
Page 159
A number of options shows up which is qualitatively of the same order as the
number of degrees of freedom of a spinor field , when one goes to the virtual
foam - like space of quantum geometrodynamics . It is difficult to say anything
more ...
A number of options shows up which is qualitatively of the same order as the
number of degrees of freedom of a spinor field , when one goes to the virtual
foam - like space of quantum geometrodynamics . It is difficult to say anything
more ...
Page 253
Mott scattering can lead to an asymmetry only if the electrons show transverse
polarization . Thus , since electrons from 3 - decay originally show longitudinal
polarization , this polarization has to be transformed first to transverse
polarization ...
Mott scattering can lead to an asymmetry only if the electrons show transverse
polarization . Thus , since electrons from 3 - decay originally show longitudinal
polarization , this polarization has to be transformed first to transverse
polarization ...
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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