Proceedings of the International School of Physics "Enrico Fermi.", Volume 49N. Zanichelli, 1971 - Nuclear physics |
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Page 14
... transition from the sum standing on the right side of ( 8 ) ( or of ( 12 ) ) to a single member of this sum . The transition in question is usually referred to as the collapse . of the state vector - a very picturesque but not very ...
... transition from the sum standing on the right side of ( 8 ) ( or of ( 12 ) ) to a single member of this sum . The transition in question is usually referred to as the collapse . of the state vector - a very picturesque but not very ...
Page 15
... transition from the sums in ( 8 ) and ( 12 ) to a single term of these sums . The answer must be inherent in the unknown laws of the behaviour of macroscopic systems and their interaction with microscopic ones . It may be better to ...
... transition from the sums in ( 8 ) and ( 12 ) to a single term of these sums . The answer must be inherent in the unknown laws of the behaviour of macroscopic systems and their interaction with microscopic ones . It may be better to ...
Page 429
... transitions between stationary states are in some sense discrete . Thus it has no meaning to say that a system passes ... transition . 72. Wave - particle duality of the properties of matter . - Under different exper- imental conditions ...
... transitions between stationary states are in some sense discrete . Thus it has no meaning to say that a system passes ... transition . 72. Wave - particle duality of the properties of matter . - Under different exper- imental conditions ...
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