Entanglement between accelerated probes in de Sitter spacetime varies independently with acceleration and curvature depending on detector motion configurations, unlike the single-probe effective-acceleration mapping.
The 4 and 5 accelerations are related by, a1 = a2 = a; q1 = −q2 = q
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Entanglement between accelerated probes in a de Sitter spacetime
Entanglement between accelerated probes in de Sitter spacetime varies independently with acceleration and curvature depending on detector motion configurations, unlike the single-probe effective-acceleration mapping.