Abstract
Starting from a “singlet” state vector for two correlated systems we find an observable whose expectation is 3 according to quantum mechanics, while it has a maximum value of 1 if only state vectors of the first type are considered. This allows a much easier experimental check of the hitherto unobserved state vectors of the second type than suggested by Bell's inequality.
Similar content being viewed by others
References
Bell, J. S. (1963).Physics,1, 1965.
Capasso, V., Fortunato, D., and Selleri, F. (1973).International Journal of Theoretical Physics,5, 319.
Clauser, J. F., Horne, M. A., Shimony, A., and Holt, R. A. (1969).Physical Review Letters,23, 880.
D'Espagnat, B. (1965).Conceptions de la physique contemporaine. (Hermann, Paris), p. 32.
Fortunato, D., and Selleri, F. (1976).International Journal of Theoretical Physics,15, 333.
Freedman, S. J., and Clauser, J. F. (1972).Physical Review Letters,28, 938.
Holt, R. A., and Pipkin, F. M. (1975). Harvard University preprint.
Horne, M. A. (1969). Thesis, Boston University (unpublished).
Jammer, M. (1974).The Philosophy of Quantum Mechanics. (John Wiley, New York).
Jauch, J. M. (1971). International School of Physics “Enrico Fermi”, Course IL,Foundations of Quantum Mechanics, D'Espagnat, D., ed. (Academic Press, New York), p. 20.
Wigner, E. (1970)American Journal of Physics,38, 1005.
Author information
Authors and Affiliations
Rights and permissions
About this article
Cite this article
Fortunato, D., Garuccio, A. & Selleri, F. Observable consequences from second-type state vectors of quantum mechanics. Int J Theor Phys 16, 1–6 (1977). https://doi.org/10.1007/BF01807118
Received:
Issue Date:
DOI: https://doi.org/10.1007/BF01807118