Proceedings of the International School of Physics "Enrico Fermi.", Volume 49N. Zanichelli, 1971 - Nuclear physics |
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Page 200
... shown how considerations involving the notion of state in axiomatic quantum theory can also motivate the BA hypothesis . Also , it is shown in Appendix II that any theory obeying the BA hypothesis can be put in the mathematical form of ...
... shown how considerations involving the notion of state in axiomatic quantum theory can also motivate the BA hypothesis . Also , it is shown in Appendix II that any theory obeying the BA hypothesis can be put in the mathematical form of ...
Page 206
... ( shown in Fig . 3 ) . Also , the whole » region was defined as containing events of all energies . e2 / M 0.5 55 32 1 4 0 0.5 1.0 e , / M Fig . 3. The four energy regions chosen to study the amplitude of the cosine dependence of R. The ...
... ( shown in Fig . 3 ) . Also , the whole » region was defined as containing events of all energies . e2 / M 0.5 55 32 1 4 0 0.5 1.0 e , / M Fig . 3. The four energy regions chosen to study the amplitude of the cosine dependence of R. The ...
Page 341
... shown in the Appendix . The existence of such operators unequal to 21 cannot be excluded . This will be shown by the following construction . Let [ M ] be the spectrum of M1 , and [ M ] be the spectrum of M2 . The spectrum [ M ] of M is ...
... shown in the Appendix . The existence of such operators unequal to 21 cannot be excluded . This will be shown by the following construction . Let [ M ] be the spectrum of M1 , and [ M ] be the spectrum of M2 . The spectrum [ M ] of M is ...
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