Proceedings of the International School of Physics "Enrico Fermi.", Volume 11N. Zanichelli, 1960 - Nuclear physics |
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Page 5
The Lüders theorem states that S invariance is implied by Lorentz invariance and
locality of the coupling . Hence , if the latter conditions are $ 1 . satisfied , one has
always invariance for combined space reflection , time reversal and ...
The Lüders theorem states that S invariance is implied by Lorentz invariance and
locality of the coupling . Hence , if the latter conditions are $ 1 . satisfied , one has
always invariance for combined space reflection , time reversal and ...
Page 32
If this quantity changes sign under time reversal ( which , according to Table I
means that it contains an odd number of factors ) its being « observed » ( in a
sense requiring additional interpretation ( * ) ) means violation of invariance
under time ...
If this quantity changes sign under time reversal ( which , according to Table I
means that it contains an odd number of factors ) its being « observed » ( in a
sense requiring additional interpretation ( * ) ) means violation of invariance
under time ...
Page 37
The reflected situation is shown in Fig . 5b : the orientation of the initial spins is
the same ; the direction of the momentum of the decay products is reversed .
What matters is , because of rotational invariance , the angle between the
direction of ...
The reflected situation is shown in Fig . 5b : the orientation of the initial spins is
the same ; the direction of the momentum of the decay products is reversed .
What matters is , because of rotational invariance , the angle between the
direction of ...
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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