Proceedings of the International School of Physics "Enrico Fermi.", Volume 49N. Zanichelli, 1971 - Nuclear physics |
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Page 33
... represented by a complex Hilbert - space of dimension 2. We denote by u + and u the normalized eigenvectors of the 3 - component of the spin for the first system and by v + and v- the corresponding eigenvectors for the second system ...
... represented by a complex Hilbert - space of dimension 2. We denote by u + and u the normalized eigenvectors of the 3 - component of the spin for the first system and by v + and v- the corresponding eigenvectors for the second system ...
Page 164
... represents a sharp space- time localization , thereby allowing the formulation of causality . Of course , as is familiar ... represented by suitably constructed wave packets , slightly above the threshold for the production of one -meson ...
... represents a sharp space- time localization , thereby allowing the formulation of causality . Of course , as is familiar ... represented by suitably constructed wave packets , slightly above the threshold for the production of one -meson ...
Page 222
... represented in the superposition ( 2.1 ) , in each of which the measurement has yielded a different outcome . If we are to follow EVERETT in letting the formalism tell its own story , without benefit of a priori metaphysics , then we ...
... represented in the superposition ( 2.1 ) , in each of which the measurement has yielded a different outcome . If we are to follow EVERETT in letting the formalism tell its own story , without benefit of a priori metaphysics , then we ...
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