Proceedings of the International School of Physics "Enrico Fermi.", Volume 11N. Zanichelli, 1960 - Nuclear physics |
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Page 338
First let us see what pairs of leptons are coupled . For the pair ( BA ) we call AQ =
( : - the transfer of charge for the pair . Now ( Wu ) , ( ve ) with AQ = + 1 already
appear in ( 12 ) . The neutral pairs ( üe ) , ( iv ) , ( ēe ) and ( ) cannot all be
coupled ...
First let us see what pairs of leptons are coupled . For the pair ( BA ) we call AQ =
( : - the transfer of charge for the pair . Now ( Wu ) , ( ve ) with AQ = + 1 already
appear in ( 12 ) . The neutral pairs ( üe ) , ( iv ) , ( ēe ) and ( ) cannot all be
coupled ...
Page 387
Theoretical properties of internally converted pairs . At high energies the
properties of the pairs are essencially independent of the origin , but differ
appreciably from those of externally produced pairs . It will be recalled that
external pairs are ...
Theoretical properties of internally converted pairs . At high energies the
properties of the pairs are essencially independent of the origin , but differ
appreciably from those of externally produced pairs . It will be recalled that
external pairs are ...
Page 388
07 + - The theme pictures , which contain x probably about 100 000 single pairs .
These can . not all be measured . The analysis of the single pairs is being
pursued by Tip ettern SAMIOS . He has selected a fiducial region far enough from
the ...
07 + - The theme pictures , which contain x probably about 100 000 single pairs .
These can . not all be measured . The analysis of the single pairs is being
pursued by Tip ettern SAMIOS . He has selected a fiducial region far enough from
the ...
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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