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Direct semi-classical/non-relativistic limit of massive Klein–Gordon–Maxwell to Vlasov–Poisson

Establish the combined semi-classical and non-relativistic limit of the (3+1)-dimensional massive Klein–Gordon–Maxwell equations and prove convergence, in an appropriate topology for observables (density, current, electromagnetic field), to the Vlasov–Poisson system. Precisely, show that under a simultaneous regime where the Planck parameter tends to zero and the speed-of-light scaling yields the non-relativistic limit, solutions of the massive Klein–Gordon–Maxwell equations converge to solutions of Vlasov–Poisson without passing through the intermediate Schrödinger–Poisson system.

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Background

The paper reviews known limits between quantum and kinetic/fluid models. It is classical that massive Klein–Gordon–Maxwell (mKGM) converges to Schrödinger–Poisson (SP) in the non-relativistic limit, and that SP converges to Vlasov–Poisson (VP) in the semi-classical limit. The authors highlight the absence of a direct result that bypasses SP and establishes a combined semi-classical/non-relativistic limit from mKGM straight to VP.

They reference analogous double-limit results for related systems (e.g., Dirac–Maxwell to SP) and note this direct limit remains unproved for mKGM. A rigorous formulation would require specifying the joint scaling, functional framework, and convergence of key observables.

References

The point 3) is not proved yet as far as we know, but we refer to for the proof of the semiclassical non-relativistic limit of the Dirac-Maxwell system to the Schr\"odinger-Poisson system.