Proceedings of the International School of Physics "Enrico Fermi.", Volume 11N. Zanichelli, 1960 - Nuclear physics |
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Page 276
This agreement between theory and experiment fails partly due to experimental
difficulties at low energies . For historical reasons it has become customary to fit
experimental ß - spectra to the Fermi spectrum multiplied by ( 1 + b / W ) since
this ...
This agreement between theory and experiment fails partly due to experimental
difficulties at low energies . For historical reasons it has become customary to fit
experimental ß - spectra to the Fermi spectrum multiplied by ( 1 + b / W ) since
this ...
Page 284
Circular polarization experiments have been performed in four sp different ways .
In one type of experiment , discussed in Section 4 ' 3 , the excess wriz attenuation
of a y - ray due to the term eq . ( 6 ) is measured . In the other three , phot one ...
Circular polarization experiments have been performed in four sp different ways .
In one type of experiment , discussed in Section 4 ' 3 , the excess wriz attenuation
of a y - ray due to the term eq . ( 6 ) is measured . In the other three , phot one ...
Page 382
The experimental result , except for those of the Los Alamos group , represent
capture rates to the sum of all bound states of 12B , not only the ... The Los
Alamos experiments indicate however that excited states contribute less than ~
10 % ...
The experimental result , except for those of the Los Alamos group , represent
capture rates to the sum of all bound states of 12B , not only the ... The Los
Alamos experiments indicate however that excited states contribute less than ~
10 % ...
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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