A freely falling quantum detector's transition rate distinguishes the RP2 geon from the spinless BTZ black hole, revealing hidden interior topology through amplitude differences and glitches.
Static, stationary and inertial Unruh-DeWitt detectors on the BTZ black hole
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abstract
We examine an Unruh-DeWitt particle detector coupled to a scalar field in three-dimensional curved spacetime. We first obtain a regulator-free expression for the transition probability in an arbitrary Hadamard state, working within first-order perturbation theory and assuming smooth switching, and we show that both the transition probability and the instantaneous transition rate remain well defined in the sharp switching limit. We then analyse a detector coupled to a massless conformally coupled field in the Hartle-Hawking vacua on the Banados-Teitelboim-Zanelli black hole, under both transparent and reflective boundary conditions at the infinity. A selection of stationary and freely-falling detector trajectories are examined, including the co-rotating trajectories, for which the response is shown to be thermal. Analytic results in a number of asymptotic regimes, including those of large and small mass, are complemented by numerical results in the interpolating regimes. The boundary condition at infinity is seen to have a significant effect on the transition rate.
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Deep in the knotted black hole
A freely falling quantum detector's transition rate distinguishes the RP2 geon from the spinless BTZ black hole, revealing hidden interior topology through amplitude differences and glitches.