Search Results
Search type | Search syntax |
---|---|
Tags | [tag] |
Exact | "words here" |
Author |
user:1234 user:me (yours) |
Score |
score:3 (3+) score:0 (none) |
Answers |
answers:3 (3+) answers:0 (none) isaccepted:yes hasaccepted:no inquestion:1234 |
Views | views:250 |
Code | code:"if (foo != bar)" |
Sections |
title:apples body:"apples oranges" |
URL | url:"*.example.com" |
Saves | in:saves |
Status |
closed:yes duplicate:no migrated:no wiki:no |
Types |
is:question is:answer |
Exclude |
-[tag] -apples |
For more details on advanced search visit our help page |
This tag is for questions regarding to the Unruh effect (also known as the Fulling–Davies–Unruh effect), the hypothetical prediction that an accelerating observer will observe a thermal bath, like blackbody radiation, whereas an inertial observer would observe none. It was described by Stephen Fulling in 1973, Paul Davies in 1975, and William Unruh in 1976.
1
vote
Static Patch Decomposition of Bunch-Davies Vacuum
I am unable to write this as a comment as my reputation isn't quite high enough.
However, Sections 1 and 2 of this paper https://arxiv.org/pdf/hep-th/0212209 discuss this as well as, to a lesser exten …
2
votes
How does Sean Carroll swap the operators and sign on the index when calculating the observed...
As you wrote, we have the operators
$$
{\hat{b}_k}^{(1)}~=~\frac{1}{\sqrt{2\sinh\left(\frac{\pi\omega}{a}\right)}}\left(\mathrm{e}^{\pi\omega/(2a)}{\hat{c}_k}^{(1)}+\mathrm{e}^{-\pi\omega/(2a)}{{\hat{ …