Proceedings of the International School of Physics "Enrico Fermi.", Volume 49N. Zanichelli, 1971 - Nuclear physics |
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Page 161
... weak interactions , it is plausible that it can be accounted for by an effective interaction bilinear in the pion fields . This being the case , the amplification device referred to above can be envisaged to work for the pions in a way ...
... weak interactions , it is plausible that it can be accounted for by an effective interaction bilinear in the pion fields . This being the case , the amplification device referred to above can be envisaged to work for the pions in a way ...
Page 162
... weak final interaction . The former does apparently not endanger the success of the set - up , since thе л - л рhase ... interactions are concerned , we have to face the problem of recombination of the pions to form kaons again . However ...
... weak final interaction . The former does apparently not endanger the success of the set - up , since thе л - л рhase ... interactions are concerned , we have to face the problem of recombination of the pions to form kaons again . However ...
Page 335
... weak interactions . However , in our case problems of quantum- mechanical measurability play a decisive role , and without the electromagnetic interaction ( i.e. without a long - range interaction having classical limit ) the very ...
... weak interactions . However , in our case problems of quantum- mechanical measurability play a decisive role , and without the electromagnetic interaction ( i.e. without a long - range interaction having classical limit ) the very ...
Contents
E WIGNER | 1 |
Comparison between gravity and electromagnetism | 7 |
233 | 54 |
Copyright | |
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A₁ angular momentum Araki-Yanase assume assumption atom axiomatic axioms BOHR cas pur classical physics commute components Compton scattering concept considered corpuscule correlation corresponding coupling d'une defined definite denote density matrix described discussion dynamical E. P. WIGNER eigenvalues eigenvectors ensemble être existence experimental fact field finite formalism given Green's function hence hidden variables hidden-variable theories Hilbert space initial interaction interpretation JAUCH l'ensemble l'onde L₁ linear mathematical measuring process mélange ment NEUMANN object observable obtained orthogonal particle peut photons Phys Poisson bracket polarization position possible postulate probabilité problem properties proposition quantal systems quantum mechanics quantum theory question relation result satisfy scattering Schrödinger equation Sect self-adjoint self-adjoint operators spin subspaces subsystem superposition system and apparatus test body theorem tion uncertainty unitary unitary operator valeurs vecteur d'état vector wave function WIGNER YANASE yes-no experiments