Proceedings of the International School of Physics "Enrico Fermi.", Volume 49N. Zanichelli, 1971 - Nuclear physics |
From inside the book
Results 1-3 of 68
Page 339
... effect in Ludwig's axiomatical system . In case of FF it represents a decision effect in Ludwig's , or a proposi- tion in Jauch and Piron's axiomatics . If the value q of O is a classical property of the apparatus which can be observ ...
... effect in Ludwig's axiomatical system . In case of FF it represents a decision effect in Ludwig's , or a proposi- tion in Jauch and Piron's axiomatics . If the value q of O is a classical property of the apparatus which can be observ ...
Page 407
... effects and observables . We will adopt the same notation as Prof. LUDWIG did in his lectures and will work in the same frame of axiomatics . So I denotes the set of effects F. An effect FeÎ represents an equivalence class of signal ...
... effects and observables . We will adopt the same notation as Prof. LUDWIG did in his lectures and will work in the same frame of axiomatics . So I denotes the set of effects F. An effect FeÎ represents an equivalence class of signal ...
Page 409
... effects F1X1 of one physical system are coexistent with all effects 1X F2 of the other system . 1 2 1 The inverse statement that two coexistent effects commute is not true in general , but it holds if one effect , say F1 , is a decision ...
... effects F1X1 of one physical system are coexistent with all effects 1X F2 of the other system . 1 2 1 The inverse statement that two coexistent effects commute is not true in general , but it holds if one effect , say F1 , is a decision ...
Contents
E WIGNER | 1 |
Comparison between gravity and electromagnetism | 7 |
233 | 54 |
Copyright | |
38 other sections not shown
Other editions - View all
Common terms and phrases
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