Unruh Effect: When Does an Object Receive Radiation?

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Discussion Overview

The discussion centers on the Unruh effect, specifically addressing when an object receives Unruh radiation upon acceleration. Participants explore the implications of the Rindler horizon's visibility and its relevance to the detection of radiation, as well as connections to cosmological horizons and their influence during the inflation era.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation

Main Points Raised

  • Some participants propose that an object receives Unruh radiation immediately upon assuming an accelerating frame, while others suggest there is a delay due to the time it takes for photons to travel from the Rindler horizon.
  • There is a question about whether Unruh radiation can be detected if the Rindler horizon is obscured, with some arguing that the horizon is not essential for the effect.
  • One participant clarifies that the temperature associated with Unruh radiation arises locally from acceleration, and the Rindler horizon is a nonessential parameter.
  • Another participant adds a caveat that while the effect is local in space, it is not completely local in time, as sustained acceleration is necessary for a thermal spectrum.
  • Discussion also touches on the relevance of cosmological horizons in the context of radiation in an expanding universe, with some asserting that unlike the Rindler horizon, the cosmological horizon is significant for radiation detection.
  • Speculation arises regarding the impact of radiation from cosmological horizons during the inflation era and its potential influence on the inflation process itself.

Areas of Agreement / Disagreement

Participants express differing views on the necessity of the Rindler horizon for detecting Unruh radiation, with some asserting it is nonessential while others maintain it plays a role. The discussion remains unresolved regarding the implications of cosmological horizons and their effects during inflation.

Contextual Notes

There are limitations regarding the assumptions made about the visibility of horizons and the conditions under which Unruh radiation is detected. The discussion also highlights the dependence on definitions of local effects in space and time.

tzimie
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When an object starts accelerating, when does it receive Unruh radiation?

1. After some delay, because it takes time for the photons to travel from the Rindler horizon
2. Immediately, because an object instantly "assumes" an accelerating frame, which is already filled with Unruh radiation.

Thanks.
 
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Demystifier said:
Number 2.

So we detect Unruh radiation even if Rindler horizon is not visible - say, is obscured by something?
 
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That's logically the same as "Can I still see something when my hands are covering my eyes?"
 
Vanadium 50 said:
That's logically the same as "Can I still see something when my hands are covering my eyes?"

What if your hands (screen) are far enough from you - almost at Rindler's horizon?
Then saying that distant screen blocks Unruh radiation is the same as claiming #1 in my first post.
 
tzimie said:
So we detect Unruh radiation even if Rindler horizon is not visible - say, is obscured by something?
That's correct. The horizon is not essential for the Unruh effect. See e.g.
http://lanl.arxiv.org/abs/gr-qc/0103108 [Mod.Phys.Lett.A16:579-581,2001]
 
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Thanks Demy! It's good to have that point clarified!
So (and please correct this if it's wrong) the temperature arises locally in the vacuum just from acceleration---and the Rindler horizon is a nonessential descriptive parameter of the acceleration?

Thanks also to Tzimie for asking the right question to elicit the clarification.
 
marcus said:
So (and please correct this if it's wrong) the temperature arises locally in the vacuum just from acceleration---and the Rindler horizon is a nonessential descriptive parameter of the acceleration?
That's almost correct, with a caveat that the effect is local in space (a very small detector can see the effect) but not completely local in time (in order for the detector response to have a thermal spectrum, the acceleration must exist for a long time).

Incidentally, today a new paper appeared which discusses these things in more detail:
http://lanl.arxiv.org/abs/1501.00119
 
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Demystifier said:
That's almost correct, with a caveat that the effect is local in space (a very small detector can see the effect) but not completely local in time (in order for the detector response to have a thermal spectrum, the acceleration must exist for a long time).

Incidentally, today a new paper appeared which discusses these things in more detail:
http://lanl.arxiv.org/abs/1501.00119
Yes! I saw that and logged it on the biblio thread! Nicolaevici "Unruh effect without Rindler horizon"! just what you were talking about (and wrote about several years ago.
 
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Thank you, and I am happy because my intuition was right :)
What's about radiation from the cosmological horizons in our expanding Universe? Do we need to see cosmological horizons or not?
 
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tzimie said:
Thank you, and I am happy because my intuition was right :)
What's about radiation from the cosmological horizons in our expanding Universe? Do we need to see cosmological horizons or not?
Unlike Rindler horizon, the cosmological horizon (similarly to the black hole horizon) is quite relevant for the radiation.
 
  • #12
I was also wondering

During the inflation era when the expansion was so rapid --> cosmological horizons were so close --> radiation from them was so intense --> average density of energy could be significant to influence and even to cancel the inflation?
 

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