Self-consistent initial-data conjecture for semiclassical gravity

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Let C\mathcal{C} be a Cauchy surface with classical initial data consisting of the induced metric habh_{ab}, extrinsic curvature KabK_{ab}, and its first two normal-time derivatives  \mathchar′26d Kab\,{\mathchar'26\mkern-12mud}\, K_{ab} and  \mathchar′26d 2Kab\,{\mathchar'26\mkern-12mud}\,^2 K_{ab}. Equivalently, prescribe the metric time derivatives gab∣Cg_{ab}|_{\mathcal{C}}, g˙ab∣C\dot g_{ab}|_{\mathcal{C}}, gab(2)∣Cg^{(2)}_{ab}|_{\mathcal{C}}, and gab(3)∣Cg^{(3)}_{ab}|_{\mathcal{C}}, together with the approximating quantities Σ\Sigma,  \mathchar′26d Σ\,{\mathchar'26\mkern-12mud}\,\Sigma,  \mathchar′26d 2Σ\,{\mathchar'26\mkern-12mud}\,^2\Sigma, UU, and VV.

Self-consistent initial-data conjecture. Self-consistent initial data for the fourth-order time derivatives of the metric can be obtained from these classical initial data by solving the fourth-order terms, namely ∇n3Ka′b′∼gab(4)∣C\nabla_n^3K_{a'b'}\sim g^{(4)}_{ab}|_{\mathcal{C}}, using the semiclassical Einstein equation. Furthermore, higher-order time derivatives of the induced metric can be obtained by formally differentiating the semiclassical Einstein equation and applying the same procedure.

This conjecture recasts the proposed zeroth-stage construction of the surface Hadamard condition for the initial-value problem of semiclassical gravity. It asserts that the missing fourth time derivative, and subsequently higher derivatives, can be determined recursively from classical initial data and the semiclassical Einstein equation; the supplied context does not establish the conjecture or give a resolution status.

References

Primary source

Benito A. Juárez-Aubry, Bernard S. Kay, Tonatiuh Miramontes and Daniel Sudarsky, “The Hadamard condition on a Cauchy surface and the renormalized stress-energy tensor”, arXiv:2406.01498 (2024).

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