We revisit the definition of the temperature of a causal diamond for the case of a free massless scalar field. The stress is given to the intrinsic, direction-dependent character of this definition. Some important limits are also discussed.

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22.

We restrict ourselves to the TT trajectories in the x0x1 plane. The explicit form for a more general trajectory will be more involved after a translation, but because the choice of the 1-direction is arbitrary, we do not loose any generality of the results.

23.

Recall that we are considering only the TT trajectories in x0x1 plane. So the “corners” here are actually wedge-like regions for some neighbourhood in x2, x3 directions.

24.

Here the TT trajectory that passes through z at some t, at t = 0 passes through x0(0) = 0 and r(0) = r.

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