Skip to content
aiqbench takeQuantum Computing

aiqbench analysis

This paper rigorously derives the non-relativistic limit of the Klein-Gordon field on curved spacetimes, demonstrating how gravitational bound states emerge from relativistic resonances while vacuum entanglement collapses into a product state. The work bridges algebraic quantum field theory with Newtonian gravity, providing explicit spectral corrections for static stars and black hole exteriors that are critical for understanding the interface between general relativity and non-relativistic quantum mechanics.
Source coveringarXiv
What this isA model's reading of the article and related coverage, written for aiqbench. Not the publisher's words.

Newton-Cartan limit of Klein-Gordon AQFT: gravitational atoms and the loss of vacuum entanglement

arXiv3 min read

arXiv:2604.26287v2 Announce Type: replace Abstract: We take the non-relativistic limit $c\to\infty$ of the free Klein-Gordon field on static spacetimes at three levels: one-particle resolvents, quasi-free states and the time-zero net. After subtraction of the rest energy, the one-particle Hamiltonian is an explicit function of a Schr\"odinger-type operator whose potential on the Schwarzschild exterior is exactly Newtonian. On regular static stars it converges to the Newtonian Schr\"odinger operator in norm-resolvent sense at rate $c^{-2}$, with convergence of eigenvalues and an explicit first post-Newtonian correction. On the Schwarzschild exterior the Boulware one-particle spectrum has no eigenvalues for any $c$; the convergence is strong but not in norm, the limit selects the Friedrichs realisation of the gravitational hydrogen atom, and its bound states emerge by spectral concentration. The same holds on the Reissner-Nordstr\"om exterior. In all cases the rescaled two-point functions converge to those of the Schr\"odinger-Fock vacuum. The hydrogenic states are limits of resonances: in each partial wave there is exactly one near each hydrogenic level, its real part carries the first post-Newtonian correction, and its width, proportional to $c^{-(4l+3)}$, is the one found for gravitational atoms by matched asymptotics. At the level of nets the time-zero Weyl algebra is the same for every $c$, and the vacuum and the dynamics converge on it, yet for smooth metrics the algebra of each bounded region with smooth boundary is a type III$_1$ factor at finite $c$ and a type I factor with a pure product vacuum in the limit. What collapses is the entanglement of the vacuum; thermal states in flat space and on stars survive the limit. With positivity of the energy imposed modulo the central charge, the axioms of Galilean nets hold in the limit for every static star and for Schwarzschild, and the vacuum is not separating.

Abstract:We take the non-relativistic limit $c\to\infty$ of the free Klein-Gordon field on static spacetimes at three levels: one-particle resolvents, quasi-free states and the time-zero net. After subtraction of the rest energy, the one-particle Hamiltonian is an explicit function of a Schrödinger-type operator whose potential on the Schwarzschild exterior is exactly Newtonian. On regular static stars it converges to the Newtonian Schrödinger operator in norm-resolvent sense at rate $c^{-2}$, with convergence of eigenvalues and an explicit first post-Newtonian correction. On the Schwarzschild exterior the Boulware one-particle spectrum has no eigenvalues for any $c$; the convergence is strong but not in norm, the limit selects the Friedrichs realisation of the gravitational hydrogen atom, and its bound states emerge by spectral concentration. The same holds on the Reissner-Nordström exterior. In all cases the rescaled two-point functions converge to those of the Schrödinger-Fock vacuum. The hydrogenic states are limits of resonances: in each partial wave there is exactly one near each hydrogenic level, its real part carries the first post-Newtonian correction, and its width, proportional to $c^{-(4l+3)}$, is the one found for gravitational atoms by matched asymptotics. At the level of nets the time-zero Weyl algebra is the same for every $c$, and the vacuum and the dynamics converge on it, yet for smooth metrics the algebra of each bounded region with smooth boundary is a type III$_1$ factor at finite $c$ and a type I factor with a pure product vacuum in the limit. What collapses is the entanglement of the vacuum; thermal states in flat space and on stars survive the limit. With positivity of the energy imposed modulo the central charge, the axioms of Galilean nets hold in the limit for every static star and for Schwarzschild, and the vacuum is not separating.

29 pages, 3 figures, 3 tables. v2: substantially revised and extended, new title (v1: "Newton-Cartan limit of Klein-Gordon AQFT and the collapse of Galilean modular structure"). Corrects the claim of v1 that the Boulware vacuum tends to the hydrogenic ground state

arXiv:2604.26287 [quant-ph]

(or arXiv:2604.26287v2 [quant-ph] for this version)

Full text under the publisher's open licence · 341 words

Related coverage