Proceedings of the International School of Physics "Enrico Fermi.", Volume 11N. Zanichelli, 1960 - Nuclear physics |
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Page 214
factors , which can be reduced by the addition theorem : DIAPE Dy D ' ) ; - M , = E
( J , M , J ' - M1kx ) ( J , M , , Ji - - M 15 , D x ( 0 ) ) . Even We may now introduce a
linking factor for particle 2 , analogous to the quantity ý defined by eq .
factors , which can be reduced by the addition theorem : DIAPE Dy D ' ) ; - M , = E
( J , M , J ' - M1kx ) ( J , M , , Ji - - M 15 , D x ( 0 ) ) . Even We may now introduce a
linking factor for particle 2 , analogous to the quantity ý defined by eq .
Page 231
In the definition of the coefficients w , we have omitted a factor Î Ì which ( like other
omitted factors ) only affects the absolute normalization . Eq . ( 94 ) exhibits , for
each type of interaction ( 1 = 0 , 1 ) , a splitting of the partial amplitude into two ...
In the definition of the coefficients w , we have omitted a factor Î Ì which ( like other
omitted factors ) only affects the absolute normalization . Eq . ( 94 ) exhibits , for
each type of interaction ( 1 = 0 , 1 ) , a splitting of the partial amplitude into two ...
Page 235
We are now left with a summation over j ; as suggested by the fact that the sign
factor ( - - ) 0 " contains ( - ) - , this will lead to a new X - symbol , riz . ir li ri k ? ? - ;
- ; IT / e J - I his 1 The final result is the simple and elegant formula ( 101 ) 11 khi ll
...
We are now left with a summation over j ; as suggested by the fact that the sign
factor ( - - ) 0 " contains ( - ) - , this will lead to a new X - symbol , riz . ir li ri k ? ? - ;
- ; IT / e J - I his 1 The final result is the simple and elegant formula ( 101 ) 11 khi ll
...
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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