Back-action from Unruh-DeWitt detectors produces energy fluxes that exactly account for detector transitions due to the Unruh effect, including negative energy density regions near the Rindler horizon and in the far future for ground-state accelerated detectors.
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The Minkowski vacuum is not exactly a thermofield-double state; explicit correlator mismatches and an alternate non-thermal entangled representation demonstrate that TFD structure arises from the derivation method rather than being fundamental.
Derives Frenet-Serret equations for relativistic motion with variable proper acceleration and torsion, relating parameters to four-jerk and four-snap via Gram-Schmidt tetrad, with analytic examples.
citing papers explorer
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Back-action from inertial and non-inertial Unruh-DeWitt detectors revisited in covariant perturbation theory
Back-action from Unruh-DeWitt detectors produces energy fluxes that exactly account for detector transitions due to the Unruh effect, including negative energy density regions near the Rindler horizon and in the far future for ground-state accelerated detectors.
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On the Limits of the Thermofield-Double Interpretation of the Minkowski Vacuum
The Minkowski vacuum is not exactly a thermofield-double state; explicit correlator mismatches and an alternate non-thermal entangled representation demonstrate that TFD structure arises from the derivation method rather than being fundamental.
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Frenet-Serret equations with variable proper acceleration in Minkowski spacetime
Derives Frenet-Serret equations for relativistic motion with variable proper acceleration and torsion, relating parameters to four-jerk and four-snap via Gram-Schmidt tetrad, with analytic examples.