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A. Beskow and J. Nilsson, Ark. Fys. 34, 561 (1967): L.A. Khalfin, Zh. Éksp. Teor. Fiz. Pis'ma Red. 8, 106 (1968) [JETP Lett. 8, 65 (1968)]; L. Fonda, G.C. Ghirardi, A. Rimini, and T. Weber, Nuovo Cimento A 15, 689 (1973); 18, 805 (1973).
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A. Beskow and J. Nilsson, Ark. Fys. 34, 561 (1967): L.A. Khalfin, Zh. Éksp. Teor. Fiz. Pis'ma Red. 8, 106 (1968) [JETP Lett. 8, 65 (1968)]; L. Fonda, G.C. Ghirardi, A. Rimini, and T. Weber, Nuovo Cimento A 15, 689 (1973); 18, 805 (1973).
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Fonda, L.1
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Rimini, A.3
Weber, T.4
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5
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51249189512
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A. Beskow and J. Nilsson, Ark. Fys. 34, 561 (1967): L.A. Khalfin, Zh. Éksp. Teor. Fiz. Pis'ma Red. 8, 106 (1968) [JETP Lett. 8, 65 (1968)]; L. Fonda, G.C. Ghirardi, A. Rimini, and T. Weber, Nuovo Cimento A 15, 689 (1973); 18, 805 (1973).
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0003691144
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M. L. Stich and M. Bass, Laser Handbook (North-Holland, Amsterdam, 1985), Chap. 4; A. Yariv and P. Yeh, Optical Waves in Crystals (Wiley, New York, 1984); B. E. A. Saleh and M. C. Teich, Fundamentals of Photonics (Wiley, New York, 1991), Sec. 7.4.B.
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17
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0343034703
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note
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Other choices of the initial state are possible as well. Different input states of mode b then correspond to different input states of the pointer of a measuring apparatus.
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18
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0343906258
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note
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In the regime of very large κ, however, the coupled mode theory breaks down and some other experimental realization of the Hamiltonian (1) should be found.
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19
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0343470511
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private communication
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The possibility of the existence of an observable playing a role similar to the phase in Ref. [4], and yielding some information about the place of down-conversion is not excluded, though; A. Luis (private communication).
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Luis, A.1
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20
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