Proceedings of the International School of Physics "Enrico Fermi.", Volume 11N. Zanichelli, 1960 - Nuclear physics |
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Page 74
say the magnetic field : ( 11 ) H ( la ) , H ( 20 ) , H ( ) , . . . . In this description the
wave function for the ground state takes the form ( 12 ) 1 [ H ( 1 ) H ( 2 ) x = N exp
| - 1673hel - ( 2 ) d ' a , dʻx . - Although the representations ( 8 ) , ( 9 ) , ( 11 ) are ...
say the magnetic field : ( 11 ) H ( la ) , H ( 20 ) , H ( ) , . . . . In this description the
wave function for the ground state takes the form ( 12 ) 1 [ H ( 1 ) H ( 2 ) x = N exp
| - 1673hel - ( 2 ) d ' a , dʻx . - Although the representations ( 8 ) , ( 9 ) , ( 11 ) are ...
Page 85
A few comments may be made about the complexion of an electromagnetic field .
When a = 0 , the field { e = } , 0 , 0 ; h = 0 , 0 , 0 } may be said to have a « purely
electric complexion » . If regarded from a reference system other than the ...
A few comments may be made about the complexion of an electromagnetic field .
When a = 0 , the field { e = } , 0 , 0 ; h = 0 , 0 , 0 } may be said to have a « purely
electric complexion » . If regarded from a reference system other than the ...
Page 161
When the neutrino field is regarded as a foreign object in a pre - existing space -
time geometry , and when that geometry is idealized as nearly flat , then it is
possible to analyze the states of excitation of this field into normal modes in a
familiar ...
When the neutrino field is regarded as a foreign object in a pre - existing space -
time geometry , and when that geometry is idealized as nearly flat , then it is
possible to analyze the states of excitation of this field into normal modes in a
familiar ...
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Contents
GENERALITĄ | 1 |
PARTE PRIMA Problemi teorici | 9 |
PARTE SECONDA Correlazioni angolari polarizzazioni e decadimenti beta | 197 |
4 other sections not shown
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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