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This research presents a novel analytical framework for solving the Schrödinger equation exactly using classical least action principles and harmonic coordinate transformations, even for systems with arbitrary nonlinear potentials. By mapping complex nonlinear problems to quadratic oscillators, the method offers an exact alternative to standard perturbation theory for cases like quartic potentials or the nonlinear pendulum where analytic solutions were previously unavailable.
Exact computation of quantum wave functions for nonlinear potentials
arXiv:2609.14480v1 Announce Type: new Abstract: Recent work shows that the Schroedinger equation can be solved exactly based only on classical least action rspa.2025.0413. The computation is based on first solving a Hamilton-Jacobi equation for the action, computing the classical propagated density along all stationary action paths, and finally constructing the exact kernel and wave function based on these classical quantities alone. The method requires that the propagated classical square root density along each stationary action path is harmonic (where a sufficient condition is that the Laplacian of the propagated action is purely time-varying), as is the case for basic examples such as the double-slit, quantum tunneling, the Einstein-Podolsky-Rosen experiment, or also as discussed here the relativistic propagator of a Higgs boson. This density is fundamentally different from using the Madelung density, which is the norm of an existing overall quantum wave. In the case of arbitrary nonlinear potentials, this condition can still be verified without loss of generality, by using a harmonic coordinate transformation and an associated time scaling for the propagated classical density and quantum wave, as this paper details. The resulting quantum wave of the time-scaled Schroedinger equation is equivalent to the quantum wave of the original Schroedinger equation, extending a standard result of Duru and Kleinert. Hence, in principle it can replace the approximations of quantum perturbation theory. For 1 to 3-dimensional systems, this harmonic coordinate change transforms a nonlinear potential into the quadratic potential of a linear oscillator, for which an exact analytic action and wave solution are already known. This makes the construction of the quantum wave beyond the hydrogen wave straightforward for basic cases where no exact solution has been derived, such as the quartic potential or the nonlinear pendulum.
Abstract:Recent work shows that the Schroedinger equation can be solved exactly based only on classical least action rspa.2025.0413. The computation is based on first solving a Hamilton-Jacobi equation for the action, computing the classical propagated density along all stationary action paths, and finally constructing the exact kernel and wave function based on these classical quantities alone. The method requires that the propagated classical square root density along each stationary action path is harmonic (where a sufficient condition is that the Laplacian of the propagated action is purely time-varying), as is the case for basic examples such as the double-slit, quantum tunneling, the Einstein-Podolsky-Rosen experiment, or also as discussed here the relativistic propagator of a Higgs boson. This density is fundamentally different from using the Madelung density, which is the norm of an existing overall quantum wave. In the case of arbitrary nonlinear potentials, this condition can still be verified without loss of generality, by using a harmonic coordinate transformation and an associated time scaling for the propagated classical density and quantum wave, as this paper details. The resulting quantum wave of the time-scaled Schroedinger equation is equivalent to the quantum wave of the original Schroedinger equation, extending a standard result of Duru and Kleinert. Hence, in principle it can replace the approximations of quantum perturbation theory. For 1 to 3-dimensional systems, this harmonic coordinate change transforms a nonlinear potential into the quadratic potential of a linear oscillator, for which an exact analytic action and wave solution are already known. This makes the construction of the quantum wave beyond the hydrogen wave straightforward for basic cases where no exact solution has been derived, such as the quartic potential or the nonlinear pendulum.
This paper computes exact wave functions for nonlinear potentials where they have not been analytically derived, using the action based construction from rspa.2025.0413. Examples include the quartic potential and the nonlinear pendulum
arXiv:2609.14480 [quant-ph]
(or arXiv:2609.14480v1 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2609.14480 arXiv-issued DOI via DataCite (pending registration)
Full text under the publisher's open licence · 328 words
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