<p>We study free graviton entanglement between Rindler wedges in the Minkowski vacuum state via the Euclidean path integral. We follow Kabat’s method for computing the conical entropy, using the heat kernel on the cone with the tip removed, whose resulting von Neumann entropy for photons correctly predicted electromagnetic edge modes. We find that, in addition to the bulk graviton contributions, the conical entropy has a contact term that can be attributed to a vector field anchored to the (<i>d</i> – 2)-dimensional (Euclidean) Rindler horizon whose contribution equals <i>d</i> – 2 times Kabat’s contact term for photons. We suggest that graviton edge modes are hence the <i>d</i> – 2 large diffeomorphisms which act internally within the Rindler horizon. Along the way, we address several known issues regarding graviton entanglement. We furthermore sketch how our results may be used to study edge modes in closed bosonic string theory.</p>

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Gravitons on the edge

  • Andreas Blommaert,
  • Sean Colin-Ellerin

摘要

We study free graviton entanglement between Rindler wedges in the Minkowski vacuum state via the Euclidean path integral. We follow Kabat’s method for computing the conical entropy, using the heat kernel on the cone with the tip removed, whose resulting von Neumann entropy for photons correctly predicted electromagnetic edge modes. We find that, in addition to the bulk graviton contributions, the conical entropy has a contact term that can be attributed to a vector field anchored to the (d – 2)-dimensional (Euclidean) Rindler horizon whose contribution equals d – 2 times Kabat’s contact term for photons. We suggest that graviton edge modes are hence the d – 2 large diffeomorphisms which act internally within the Rindler horizon. Along the way, we address several known issues regarding graviton entanglement. We furthermore sketch how our results may be used to study edge modes in closed bosonic string theory.