2013
DOI: 10.11648/j.ajpc.20130206.12
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The Quantum Potential: The Missing Interaction in the Density Maximum of He4 at the Lambda Point

Abstract: The lambda point in liquid He 4 is a well established phenomenon acknowledged as an example of Bose-Einstain condensation. This is generally accepted, but there are serious discrepancies between the theory and experimental results, namely the lower value of the transition temperature T λ and the negative value of dT λ /dP. These discrepancies can be explained in term of the quantum stochastic hydrodynamic analogy (SQHA). The SQHA shows that at the He 4 I →He 4 II superfluid transition the quantum coherence len… Show more

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Cited by 10 publications
(24 citation statements)
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“…However, the superposition of the global or universal wave function still exists (and remains globally coherent) [46]. This conundrum can be logically accepted using the solution proposed by Poincaré and recently extended to quantum systems [50] which shows that irreversible phenomena can occur in a global system subject to reversible behavior, since the recurrence appears over a much longer time interval than universe all life. (for example, the recurrence time provided by Boltzmann, required for a single cm 3 of gas to return to its initial state, has the order of many trillions of digits).…”
Section: Stochastic Quantum Hydrodynamic Model and The Decoherence Theorymentioning
confidence: 99%
“…However, the superposition of the global or universal wave function still exists (and remains globally coherent) [46]. This conundrum can be logically accepted using the solution proposed by Poincaré and recently extended to quantum systems [50] which shows that irreversible phenomena can occur in a global system subject to reversible behavior, since the recurrence appears over a much longer time interval than universe all life. (for example, the recurrence time provided by Boltzmann, required for a single cm 3 of gas to return to its initial state, has the order of many trillions of digits).…”
Section: Stochastic Quantum Hydrodynamic Model and The Decoherence Theorymentioning
confidence: 99%
“…The presence of the QP is needed for the realization of the quantum stationary states (i.e., eigenstates) that happen when the force of the QP exactly balances the Hamiltonian one. On the other hand, when we deal with large-scale systems with physical length c   L and when fluctuations are present in weakly interacting systems, we can have a vanishing small quantum force at large distances (see appendix A) [22,37,38] that, becoming much smaller than fluctuations, can be correctly neglected in the motion equations. It must be underlined that not all types of interactions lead to a vanishing small quantum force at large distance (a straightforward example is given by linear systems where the quantum potential owns a quadratic form (see appendix A) [22,38].…”
Section: Analysis Of Quantization Condition and Quantum Coherence In mentioning
confidence: 99%
“…It must be underlined that not all types of interactions lead to a vanishing small quantum force at large distance (a straightforward example is given by linear systems where the quantum potential owns a quadratic form (see appendix A) [22,38]. Nevertheless, it exists a large number of non-linear long-range weak potentials (e.g., Lennard Jones types) where the quantum potential tends to zero (see appendix A) at infinity and can be neglected [37]. In this case, a rarefied gas of such interacting particles behaves as a classical phase when the mean particle distance is much larger that the quantum potential range of interaction [22,37,38].…”
Section: Analysis Of Quantization Condition and Quantum Coherence In mentioning
confidence: 99%
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“…Since the invariance of light speed is the generating property of the Lorentz transformations, the co-variant form (that is, invariant 4-scalar product) of quantum potential that reads (Chiarelli, 2014b):…”
Section: Relativistic Approachmentioning
confidence: 99%