On the quantum Guerra–Morato action functional
| dc.contributor.author | Knorst, Josué | pt_BR |
| dc.contributor.author | Lopes, Artur Oscar | pt_BR |
| dc.date.accessioned | 2025-10-30T07:55:09Z | pt_BR |
| dc.date.issued | 2024 | pt_BR |
| dc.identifier.issn | 0022-2488 | pt_BR |
| dc.identifier.uri | http://hdl.handle.net/10183/298432 | pt_BR |
| dc.description.abstract | Given a smooth potential W : Tⁿ → R on the torus, the Quantum Guerra–Morato action functional is given by I (ψ) = ∫ (Dv Dv * 2 (x) − W (x) ) a (x)² dx, where ψ is described by ψ = a ei u ℏ , u = v + v * 2 , a = e v * − v 2 ℏ , v, v* are real functions, ∫a2(x)dx = 1, and D is the derivative on x ∈ Tn. It is natural to consider the constraint div(a²Du) = 0, which means flux zero. The a and u obtained from a critical solution (under variations τ) for such action functional, fulfilling such constraints, satisfy the Hamilton-Jacobi equation with a quantum potential. Denote ′ = d d τ . We show that the expression for the second variation of a critical solution is given by ∫a² D[v′] D[(v*)′] dx. Introducing the constraint ∫a² Du dx = V, we also consider later an associated dual eigenvalue problem. From this follows a transport and a kind of eikonal equation. | en |
| dc.format.mimetype | application/pdf | pt_BR |
| dc.language.iso | eng | pt_BR |
| dc.relation.ispartof | Journal of mathematical physics. New York. Vol. 65, no. 8 (Aug 2024), [Art.] 082102, 12 p. | pt_BR |
| dc.rights | Open Access | en |
| dc.subject | Equacoes de Hamilton-Jacobi | pt_BR |
| dc.subject | Quantização | pt_BR |
| dc.title | On the quantum Guerra–Morato action functional | pt_BR |
| dc.type | Artigo de periódico | pt_BR |
| dc.identifier.nrb | 001210129 | pt_BR |
| dc.type.origin | Estrangeiro | pt_BR |
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