2021
DOI: 10.1007/978-3-030-80209-7_34
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From Quantum Hydrodynamics to Koopman Wavefunctions I

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Cited by 8 publications
(11 citation statements)
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“…As discussed in [23,22], the Madelung transform of complex partial differential equations simply corresponds to expressing the equation in terms of amplitude and phase by writing Ψ in polar form. In the present section, this procedure will be applied to the KvH equation.…”
Section: Madelung Transform Of the Kvh Equationmentioning
confidence: 99%
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“…As discussed in [23,22], the Madelung transform of complex partial differential equations simply corresponds to expressing the equation in terms of amplitude and phase by writing Ψ in polar form. In the present section, this procedure will be applied to the KvH equation.…”
Section: Madelung Transform Of the Kvh Equationmentioning
confidence: 99%
“…Here we recall that the Lie algebra of the central extension Diff ω (T * Q) is isomorphic to the space of functions F (T * Q). See further details in [23,22]. Then, we are left with a relation between the momentum map (3) for the classical Liouville equation and the momentum map (17) associated to the KvH Madelung transform, that is…”
Section: Madelung Transform Of the Kvh Equationmentioning
confidence: 99%
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“…For example, the Lagrange-to-Euler map (3.3) now reads D a (z, t) = ´Da,0 (z)δ(z − η(z 0 , t)) d 2 z 0 , or equivalently in terms of the Jacobian J η = det ∇η. We note that, since the χ a 's all obey the same KvH equation, the Lagrangian path η is the same for each a = 1, ..., N. Upon defining In the limit case Σ → 0, the von Neumann operator associated to the singular Wigner function W = Dδ(λ − A) was presented explicitly in [31].…”
Section: A Von Neumann Operators In Koopman Mechanicsmentioning
confidence: 99%