## Proceedings of the International School of Physics "Enrico Fermi.", Volume 11N. Zanichelli, 1960 - Nuclear physics |

### From inside the book

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Page 118

Then the three integrals ( 72 ) provide three

parameters a and B . These

a solution .

Then the three integrals ( 72 ) provide three

**functions**of the two matareparameters a and B . These

**functions**provide a ... One starts with an arbitrary**function**— in the present case the 103 .**function**t = t ( 8 ) - - and from it generatesa solution .

Page 140

In this way the wave

field becomes expressed as a

Y = N exp [ - ( 167°he ) - 1 ] H ( a ) · H ( y ) | x – y | - doxd ' y . as sur itinsic magneti

...

In this way the wave

**function**( 99 ) for the ground state of the electromagneticfield becomes expressed as a

**functional**of the magnetic field ( * ) : We : thi ( 101 )Y = N exp [ - ( 167°he ) - 1 ] H ( a ) · H ( y ) | x – y | - doxd ' y . as sur itinsic magneti

...

Page 242

The new angular

the corresponding direction of emission , such zubol ( averaging is most easily

performed if the direction in question occurs last in klor in the angular

The new angular

**functions**9 are hi Riy ka ( 122 ) kk , k , k , k , 0 % , xits . ... overthe corresponding direction of emission , such zubol ( averaging is most easily

performed if the direction in question occurs last in klor in the angular

**function**.### What people are saying - Write a review

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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