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

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Page 74

In this

( 1 ) H ( 2 ) x = N exp | - 1673hel - ( 2 ) d ' a , dʻx . - Although the representations (

8 ) , ( 9 ) , ( 11 ) are all equivalent , the first two of them depend for their ...

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 all equivalent , the first two of them depend for their ...

Page 139

In the same way the electromagnetic field in a nearly flat space - time is often

harmonic oscillators . The ground state wave function becomes a normalized

product of ...

In the same way the electromagnetic field in a nearly flat space - time is often

**described**in terms of the co - ordinates $ 1 , $ 2 , 83 , . . . of an infinite set ofharmonic oscillators . The ground state wave function becomes a normalized

product of ...

Page 150

Therefore the following brief resumé of the sum over histories and the topological

configuration of the system at the time t ' is

Therefore the following brief resumé of the sum over histories and the topological

**description**of commutators will be limited to the bare facts , plus some ... Theconfiguration of the system at the time t ' is

**described**by the single number x ' .### What people are saying - Write a review

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### Contents

GENERALITÀ | 1 |

PARTE PRIMA Problemi teorici | 9 |

PARTE SECONDA Correlazioni angolari polarizzazioni e decadimenti beta | 197 |

4 other sections not shown

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### Common terms and phrases

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 elementary elements 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 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