Null-shifted Rindler wedges yield selective non-Gibbsian thermality in one chiral sector via Bogoliubov transformations, with the global Minkowski state remaining pure.
X T u = const v = const R1 u = const v = const R2 u = const v = const R3 v-shift u-shift Accelerated Observers: Rindler-1: Rindler-2: Rindler-3: R3⊂R2⊂R1⊂M M FIG
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Four inequivalent paths to Thermality in Minkowski spacetime
Null-shifted Rindler wedges yield selective non-Gibbsian thermality in one chiral sector via Bogoliubov transformations, with the global Minkowski state remaining pure.