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Study on double-slit device with two correlated particles 35 y yM y1 >> σ0 A S1 ∼ σ0 2σ0 x yN B 8 ∼σ 0 t=0 D S2 Fig. 2: Schematic drawing of a two-slit device in which two identical disentangled particles are simultaneously emitted by the source S1 . The symmetrical detection is not predicted at the central maximum, using both SQM and BQM. But, using BQM, we can have symmetrical detection at the other maxima (for example, at y1 as the first acceptable maximum) under the condition Y ≪ 2πσ0 . mass in the y-direction.

Thus, it was impossible to discriminate between the standard and the Bohmian quantum mechanics (BQM) at the individual levels. In fact, the two theories can be discriminated at this level, because SQM is a probabilistic theory while BQM is a precisely defined and deterministic theory. In this chapter, we have studied entangled and disentangled wave functions that can be imputed to a two-particle interference device, using a Gaussian wave function as a real representation. Then, SQM and BQM predictions are compared at both the individual and the statistical levels 1 [29-30].

Two double-slit experiment using position entanglement of EPR pair 25 arXiv:quant-ph/0206196 v1 28 Jun 2002 Argon laser IF 702 nm L D MCA xxxxxxxxxxx xxxxxxxxxxx xxxxxxxxxxx xxxxxxxxxxx xxxxxxxxxxx xxxxxxxxxxx optical condenser start Silicon avalanche photodiode TAC/SCA 351 nm coincidence stop double slit xxxxxxxxxxx xxxxxxxxxxx xxxxxxxxxxx xxxxxxxxxxx xxxxxxxxxxx xxxxxxxxxxx non-linear crystal IF 702 nm L D Counter Silicon avalanche photodiode Fig. 2: The experimental apparatus. A pump laser at 351 nm generates parametric down conversion of type I in a lithium-iodate crystal.

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2D Quantum Gravity and SC at high Tc by Polyakov A.


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