Tuesday, 4 June 2013

The equation of Unruh effect

                      The Unruh temperature, derived by William Unruh in 1976, is the effective temperature experienced by a uniformly accelerating detector in a vacuum field. It is given by
T = \frac{\hbar a}{2\pi c k_\text{B}},
where a is the local acceleration, k_\text{B} is the Boltzmann constant, \hbar is the reduced Planck constant, and c is the speed of light. Thus, for example, a proper acceleration of 2.5 × 1020 m s−2 corresponds approximately to a temperature of 1 K.
The Unruh temperature has the same form as the Hawking temperature T_\text{H} = \hbar g/(2\pi c k_\text{B}) of a black hole, which was derived (by Stephen Hawking) independently around the same time. It is, therefore, sometimes called the Hawking–Unruh temperature.

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