Proceedings of the International School of Physics "Enrico Fermi.", Volume 11N. Zanichelli, 1960 - Nuclear physics |
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Page 102
Any given choice corresponds to an arbitrary way of slicing the 4 - space apart
with a curved and waving knife into a region before and a region after o . On this
surface the 9 pieces of geometrically significant information implied by ( 3 gun
and ...
Any given choice corresponds to an arbitrary way of slicing the 4 - space apart
with a curved and waving knife into a region before and a region after o . On this
surface the 9 pieces of geometrically significant information implied by ( 3 gun
and ...
Page 281
A particle with spin S possesses , in general , ( 28 + 1 ) possible orientations of its
intrinsic angular momentum with respect to a given direction . A particle beam is
called unpolarized if all of these states are equally populated . The electron , a ...
A particle with spin S possesses , in general , ( 28 + 1 ) possible orientations of its
intrinsic angular momentum with respect to a given direction . A particle beam is
called unpolarized if all of these states are equally populated . The electron , a ...
Page 327
A more severe test of the AT = į rule would be given by study of the ratio w ( K +
→ 3T ) / ( K ; 371 ) , for the [ AT ] = } rule predicts that this ratio should have the
value unity [ 50 , 64 ) . An admixture of AT1 = } transition changes this ratio to w (
K + ...
A more severe test of the AT = į rule would be given by study of the ratio w ( K +
→ 3T ) / ( K ; 371 ) , for the [ AT ] = } rule predicts that this ratio should have the
value unity [ 50 , 64 ) . An admixture of AT1 = } transition changes this ratio to w (
K + ...
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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