Can Electric Fields Affect the Unruh Temperature of Vacuum Fluctuations?

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Discussion Overview

The discussion revolves around the potential influence of electric fields on the Unruh temperature associated with vacuum fluctuations. Participants explore the relationship between electric fields, particle creation, and the Unruh effect, as well as the distinctions between the Unruh effect and the Schwinger effect.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation

Main Points Raised

  • One participant presents the Unruh temperature formula and suggests that applying an electric field could alter the annihilation time of electron-positron pairs, potentially allowing for measurement of the temperature.
  • Another participant argues that the creation of electron-positron pairs in the presence of an electric field is more accurately described by the Schwinger effect rather than the Unruh effect.
  • A further comment questions the energy source for particle production in the context of electric fields, suggesting that photons might be produced instead of electron-positron pairs if the field strength is below a certain threshold.
  • One participant emphasizes that the Unruh effect is fundamentally tied to acceleration and that only an accelerated observer would detect Unruh radiation, challenging the heuristic description of particle creation from the vacuum.

Areas of Agreement / Disagreement

Participants express differing views on the relationship between electric fields and the Unruh effect, with some asserting that the Schwinger effect is the more relevant phenomenon in this context. The discussion remains unresolved regarding the implications of electric fields on the Unruh temperature.

Contextual Notes

There are uncertainties regarding the conditions under which particles are produced and the definitions of the effects being discussed. The relationship between electric field strength and particle creation remains ambiguous.

jcap
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The Unruh temperature is given by
$$T=\frac{\hbar\ a}{2\pi c k_B}.$$
As I understand it one can think of pairs of electrons and positrons popping out of the vacuum and then annihilating. Imagine that we apply an electric field ##\vec{E}## to a region of space. Each electron and positron would be accelerated in opposite directions parallel to the field so that they will take slightly longer to annihilate. Thus I could imagine the properties of the vacuum changing in such a circumstance. We could naively use Newton's 2nd law to find the equation of motion of an electron/positron:
$$\vec{E}\ e=m_e\ \vec{a}.$$
Substituting the magnitude of the acceleration ##a## into the Unruh formula we get
$$T=\frac{\hbar}{2\pi c k_B}\frac{E\ e}{m_e}.$$
If we take the applied electric field strength ##E=1\ \hbox{MV/m}## then the Unruh temperature is
$$T\approx 10^{-2}\ \hbox{K}.$$
Perhaps this temperature could be measured?
 
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Demystifier said:
In the absence of electric field, it's not really that electron-positron pairs pop out of the vacuum. In the presence of the field the pairs can be created, but then it is the Schwinger effect, not Unruh effect. See e.g. https://www.physicsforums.com/threads/schwinger-effect.53064/
I was thinking that if the field strength is less than the Schwinger field of ##10^{18}## V/m then maybe just photons are produced rather than electron/positron pairs. I'm not sure where the energy would come from to produce these particles - maybe from the vacuum itself?
 
jcap said:
As I understand it one can think of pairs of electrons and positrons popping out of the vacuum and then annihilating.

That's not a good heuristic description of the Unruh effect. Remember that only an accelerated observer detects Unruh radiation. The "source" of the radiation is ultimately whatever energy source is producing the acceleration--for example, the observer's rocket engine. From the standpoint of the quantum field, the radiation is produced by the interaction of the accelerated detector with the field.
 
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