Skip to content
DraconiticResearch
Search Sources API
203,203 studies31 sourcesUpdated 20 min ago
PreprintCC BY 4.0arXiv

Hadamard states for spacetimes with timelike boundaries

Abstract

We formulate and prove existence of pure quasifree Hadamard states for the Klein--Gordon field with Dirichlet boundary condition on a globally hyperbolic spacetime with timelike boundary. The microlocal condition is imposed on the one-particle Hilbert-space-valued distribution p∘ GD rather than on the two-point function. This is expressed by a b-wave-front set condition on the compressed future cone. The analysis on the manifold with corners M̅×M̅ is then almost completely avoided. We prove that our version of the Hadamard condition is universal in the class of quasi-free Hadamard states. We also prove a propagation theorem for positive-energy microlocal splittings which uses only a microlocal splitting in the small b-calculus and well-posedness of the Dirichlet problem, and in particular requires no propagation theorem for reflected or gliding rays; combined with an explicit computation in the ultrastatic case and a Fulling--Narcowich--Wald deformation argument this yields the construction of a pure quasi-free Dirichlet--Hadamard state.

Related

  1. Hadamard states for linearized gravity on asymptotically flat spacetimes
    Christian Gérard, Mikhail Molodyk, Michał Wrochna
    arXivPreprintarXiv licenceFull textAnalysis & PDEsMathematical physicsarXiv
  2. The Hadamard parametrix on globally hyperbolic spacetimes with Robin boundary conditions: Fundamental solutions and Hadamard states
    Beatrice Costeri, Claudio Dappiaggi, Benito Alberto Juárez-Aubry
    arXivPreprintCC BY 4.0Full textAnalysis & PDEsMathematical physicsarXiv
  3. Almost-splitting of spacetimes under timelike sectional curvature bounds
    Nicola Gigli, Melanie Graf, Robert J. McCann +3
    arXivPreprintCC BY 4.0Full textGeometry & topologyGravitation & general relativityarXiv
  4. A no-go theorem for closed timelike curves in globally null-foliated spacetimes
    Hongsheng Zhang
    arXivPreprintarXiv licenceFull textMathematical physicsGravitation & general relativityarXiv
  5. Why Hadamard states?
    Eleanor March
    arXivPreprintarXiv licenceFull textMathematical physicsGeneral physicsarXiv
BibTeX
@misc{contini2026hadamard,
  title = {{Hadamard states for spacetimes with timelike boundaries}},
  author = {Alessandro Pietro Contini and Alexander Strohmaier},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2609.13358},
  eprint = {2609.13358},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2609.13358},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Hadamard states for spacetimes with timelike boundaries
AU  - Alessandro Pietro Contini
AU  - Alexander Strohmaier
PY  - 2026
DA  - 2026/09/11
PB  - arXiv
DO  - 10.48550/arxiv.2609.13358
UR  - https://arxiv.org/abs/2609.13358
AB  - We formulate and prove existence of pure quasifree Hadamard states for the Klein--Gordon field with Dirichlet boundary condition on a globally hyperbolic spacetime with timelike boundary. The microlocal condition is imposed on the one-particle Hilbert-space-valued distribution p∘ G_D rather than on the two-point function. This is expressed by a b-wave-front set condition on the compressed future cone. The analysis on the manifold with corners M̅×M̅ is then almost completely avoided. We prove that our version of the Hadamard condition is universal in the class of quasi-free Hadamard states. We also prove a propagation theorem for positive-energy microlocal splittings which uses only a microlocal splitting in the small b-calculus and well-posedness of the Dirichlet problem, and in particular requires no propagation theorem for reflected or gliding rays; combined with an explicit computation in the ultrastatic case and a Fulling--Narcowich--Wald deformation argument this yields the construction of a pure quasi-free Dirichlet--Hadamard state.
ER  -