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This quantity includes lecture notes and chosen contributed papers awarded on the overseas summer season college on New advancements in Semiconductor Physics held on the collage of Szeged, July 1-6, 1979. the main a part of the contributions during this quantity is expounded to the hot experimental technics and theoretical principles utilized in study of recent semiconductor fabrics, as a rule III-V semiconductors.
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For instance, one naturally imagines that a certain "reality" lies behind the possibility of predicting with certainty the result of the next measurement of the length of an object on which many accurate measurements of the same kind were previously performed. In this case, then, there is a real property of the object that manifests itself in the predictable result of the measurement of length. 2. ELEMENTARY PROOF OF BELL'S INEQUALITY 43 entirely conventional, but also in the very notion of extension.
15. 16. 17. 18. A. EINSTEIN, 8. PODOLSKY, and N. ROSEN, Phys. Rev. 47, 777-780 (1935). N. BOHR, Phys. Rev. 48, 696-702 (1936). E. SCHROOINGER, Proc. Camb. Phil. Soc. 31,555-563 (1935). W. H. FURRY, Phys. Rev. 49, 393-399 (1936). W. H. FURRY, Phys. Rev. 49,476 (1936). E. SCHROOINGER, Proc. Camb. Phil. Soc. 32, 446-452 (1935). D. FORTUNATO, Lett. Nuovo Cim. 15,289-290 (1976). D. BOHM, Quantum Theory Prentice Hall, Englewood Cliffs, NJ (1951). D. BOHM and Y. AHARONOV, Phys. Rev. 108, 1070-1076 (1957).
In 1969, Clauser, Home, Shimony, and Holt(l7) (CHSH) suggested the use of pairs of optical photons emitted by atomic cascades. For such photons they assumed that the binary choice was between transmission and absorption in a polarizer. For every choice of the polarizer's orientations a and b, they introduced four probabilities, T(a±, b±), where, for instance, T(a+, b-) is the probability that observer 0,,- finds A(a) +1 (photon rt. transmitted through polarizer with -1 (photon ~ absorbed by polarizer with axis b) axis a) and that 0(3 finds B(b) (Fig .