Unruh effect and lessons regarding reality

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The Unruh effect claims that a quantum state which can be defined as an "empty vacuum state" by an inertial observer will become a "thermal state containing particles" for an observer with constant acceleration a; the temperature observed is T ~ a.

In contrast to other oberver dependent effects this is not just a different interpretation of one frame-independent reality but seems to be a challange for physical reality at all. Let me explain why.

Suppose we are detecting particles in different references frames, i.e. with different detectors. Each time we are detecting a particle we agree that there is a particle, but we are not in agreement regarding its energy. We are not worried about this fact b/c we can use a Lorentz transformation to get the relation between energy and momentum.

For the Unruh effect it becomes much more disturbing b/c we cannot even agree whether there there is a particle or not. So it seems that we are no longer talking about one unique quantum state with frame dependent interpretations but that we have two truly different quantum states, two different "realities". There is not one event "a particle" with different interpretations like "energies E, E', E'', ...", but there are different realities some with an event "a particle", some with "no particle".

Suppose an accelerating observer and a goup of stationary observers at rest collect the information regarding "their quantum states" over a couple minutes. Once the accelerating observer passes a stationary one they make a simultaneous measurement whether there is a particle or not. After a while the obervers at rest will not have counted any particle, but the accelerating observer will have counted many. So they disagree on the fact "whether there are particles at all".

b/c every particle can be detected only once one could get rid of the problem via the idea that the particles detected by the accelerated observer cannot be detected by the obsevers at rest, so there is no logical contradiction. This is OK, but of course the accelerating observer "knows" that there are other particles that he could detect in principle, but that they escape from his detector by whatever reason. These particles are not detected by the observers at rest, not even in principle.

So the particles detected by the accelerated observer are not and cannot be detected by the observers at rest (b/c they can be detected only once). And the particles not detected by the accelerated observer are not and need not be detected by the observers at rest. So it really seems that there is no logical contradiction - but you may understand that when talking about "reality" one may be bothered by these ideas.

Any thoughts?
 
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I am not a GR expert, but.

Let's imagine the simplest case - I have a "perfect detector" and as soon as it sees a particle, it puts up a flag. All observers agree that this flag goes up - or not- irrespective of frame. The rocket takes off, and after a moment, the flag goes up.

If you ask the rocket traveler what happened, she will say that the rocket started accelerating, they saw Unruh radiation, and the detector sent up a flag.

If you ask the stay-at-home traveler, she will say that the rocket started accelerating, began to radiate, and the detector measured this radiation and sent up a flag.

This is in one of Unruh's papers. Now, you might say, "suppose I took great care to design a rocket that had no changing multipoles and thus will not radiate". It turns out that in that case the detector will not respond to radiation. If you want the detector to be able to detect, it needs some sort of multipole to respond to the radiation, and that very multipole begins to emit. So the answer is that what one observer characterizes as absorbtion, the other characterizes as emission.
 


So it seems that we are no longer talking about one unique quantum state with frame dependent interpretations but that we have two truly different quantum states
No, it's all one state, but observers may disagree on whether it's vacuum. Different observers have different vacuums.
what one observer characterizes as absorbtion, the other characterizes as emission.
Yes, exactly.
 


Bill_K said:
No, it's all one state, but observers may disagree on whether it's vacuum.
yes, I know, sorry for the confusing formulation
 


Vanadium 50 said:
This is in one of Unruh's papers ... So the answer is that what one observer characterizes as absorbtion, the other characterizes as emission.
is this really the way to resolve the 'paradox'? thanks a lot for this information, seems quite interesting!
 
In QFT, we build the theory in terms of Poincare unirreps. As soon as you transform to an accelerating FoR, you can't expect the Poincare-based theory to remain good in all aspects.

Consider a simple uniform-acceleration case. The accelerated observer is no longer in Minkowski spacetime, but rather in Rindler spacetime, with extra horizons, etc. Imho, one should then return to a group of transformations that encompass both Poincare and uniform accelerations, then redo the Wignerian analysis from scratch with the (new) Casimirs, etc, and construct unirreps of this larger group. Without such a unified framework, the accelerated and unaccelerated observers just confuse each other.
 
strangerep said:
In QFT, we build the theory in terms of Poincare unirreps. As soon as you transform to an accelerating FoR, you can't expect the Poincare-based theory to remain good in all aspects.

Consider a simple uniform-acceleration case. The accelerated observer is no longer in Minkowski spacetime, but rather in Rindler spacetime, with extra horizons, etc. Imho, one should then return to a group of transformations that encompass both Poincare and uniform accelerations, then redo the Wignerian analysis from scratch with the (new) Casimirs, etc, and construct unirreps of this larger group. Without such a unified framework, the accelerated and unaccelerated observers just confuse each other.

Mathematically this is clear. It's a question regarding "interpretation" and "reality", not regarding the math
 
tom.stoer said:
[...] It's a question regarding "interpretation" and "reality", [...]
That's precisely the purpose of a group of transformations between reference frames. Without it, one observer's "reality" cannot be meaningfully compared with another's.
 
  • #10
Vanadium 50 said:
I am not a GR expert, but.

Let's imagine the simplest case - I have a "perfect detector" and as soon as it sees a particle, it puts up a flag. All observers agree that this flag goes up - or not- irrespective of frame.

This just shifts the issue backwards by assuming a "perfect detector that all observers agree about whether its flag is up or down".
As strangerep points out to have such an agreement a new set of transformations would be needed. And that is what Tom stoer seems to be looking for in the OP.
 
  • #11
strangerep said:
That's precisely the purpose of a group of transformations between reference frames. Without it, one observer's "reality" cannot be meaningfully compared with another's.
Sorry to say that but reality in the philosophical sense is never about an "observer's reality"; refer e.g. to Wkipedia: "... reality includes everything that is and has been, whether or not it is observable or comprehensible". What you are talking about are perceptions.

It is absolutely clear to me that we need transformations (acting on states) to compare perceptions of observers, but not to compare realities, as there is - by definition - only one reality.

This holds in non-rel. QM if one is willing to restrict the meaning of reality. Any two observers will agree on the result of a measurement (modulo some transformations) in terms of classicasl physics.

In reality there should be one particle (one event that a particle is at a certain location) or there should be no particle. And this is independent from any observer. The Unruh effect adds an additional philosophical problem b/c the "event that there is a particle" is no longer a concept of an underlying reality - b/c there are different groups of observers some detecting particles, some don't.

The idea that the "existence of a particle" is an element of reality is questioned by the Unruh effect!

This is my problem.

I see some logical excuses (e.g. that there is not one experiment but two, one for each observer, and in one experiment there is a particle whereas in the other one there isn't) but nevertheless the Unruh effect restricts the (limited) concept of reality according to non-rel. QM.
 
  • #12
tom.stoer said:
Sorry to say that but reality in the philosophical sense is never about an "observer's reality"; refer e.g. to Wkipedia: "... reality includes everything that is and has been, whether or not it is observable or comprehensible". What you are talking about are perceptions.

It is absolutely clear to me that we need transformations (acting on states) to compare perceptions of observers, but not to compare realities, as there is - by definition - only one reality.

This holds in non-rel. QM if one is willing to restrict the meaning of reality. Any two observers will agree on the result of a measurement (modulo some transformations) in terms of classicasl physics.

In reality there should be one particle (one event that a particle is at a certain location) or there should be no particle. And this is independent from any observer. The Unruh effect adds an additional philosophical problem b/c the "event that there is a particle" is no longer a concept of an underlying reality - b/c there are different groups of observers some detecting particles, some don't.

The idea that the "existence of a particle" is an element of reality is questioned by the Unruh effect!

This is my problem.

I see some logical excuses (e.g. that there is not one experiment but two, one for each observer, and in one experiment there is a particle whereas in the other one there isn't) but nevertheless the Unruh effect restricts the (limited) concept of reality according to non-rel. QM.

With that definition of reality a very simple conclusion is that particles are not real. I don't find this too disturbing, they wasn't be defined as real in the first place, particles are only our way to refer to some set of relativistic invariants.

The Unruh effect is not philosophically different to say that a field configuration appears different in different coordinates.

I think this is not so far from what happens in QFT, where field configurations change using different frame of reference. In fact a field that in some frame has a particle with momentum p in some other frame has a particle with momentum \Lambda p.
In the Unruh effect not only the momentum changes, but that's all.

To rephrase one of your quoted sentences:
The idea of the "existence of a field" is an element of reality not questioned by the Unruh effect!

Ilm
 
  • #13
Ilmrak said:
With that definition of reality a very simple conclusion is that particles are not real.
That's a way out; w/o logical inconsistencies.

Ilmrak said:
I don't find this too disturbing ...
I do ;-)

Ilmrak said:
The Unruh effect is not philosophically different to say that a field configuration appears different in different coordinates.
Really?

Ilmrak said:
In the Unruh effect not only the momentum changes, but that's all.
Yes, but for me that's more than just different momenta. Special Relativity did not really affect our concept of realitry; QM does, and QFT does even more!

Ilmrak said:
The idea of the "existence of a field" is an element of reality not questioned by the Unruh effect!
Would you really refer to a field? not just to a state?

Anyway, the concept of reality becomes even more veiled and vague ... or even void
 
  • #14
Why do you find it disturbing? Particles are not objects that exist, they are just labels/names for some of the states of the fields.
 
  • #15
It was disturbing to lose the concept of "reality of values of attributes of particles" in QM (you cannot assign attributes like spin, etc. to a particle before this atrtribute of the particle has been measured). But in QM there was no problem with the particle itself.

Now we do not only lose the concept of "reality of values of attributes of particles" but the concept of "reality of particles".

I think this *is* disturbing (when thinking about reality; if you stick to positivism there is no such problem ;-)
 
  • #16
tom.stoer said:
"The Unruh effect is not philosophically different to say that a field configuration appears different in different coordinates."

Really?

Well, it roughly says that two observers won't generally agree on the particle content of some system. Being the particle content a label to describe a fields configurations, I'd say that my sentence is not so wrong.

tom.stoer said:
"In the Unruh effect not only the momentum changes, but that's all."

Yes, but for me that's more than just different momenta. Special Relativity did not really affect our concept of reality; QM does, and QFT does even more!

Relativity does change our concept of reality (whatever it could be).

Special relativity changes for example the definition of simultaneity, which we used to think about as “real” and that is instead coordinate dependent.

General relativity shows that the gravitational field is not “real” in the sense we thought before. Two different observers won't agree on the strength of gravitational force in some point or on the gravitational energy of some system.

Roughly speaking, each time the symmetry group of our theory changes casimirs changes as well. So the value of quantity that was coordinates independent, quantity that we thought as “real”, becomes dependent by the observer point of view.

tom.stoer said:
"The idea of the "existence of a field" is an element of reality not questioned by the Unruh effect!"

Would you really refer to a field? not just to a state?

I could say “state”, but I'd have to specify that I'm talking about a coordinate independent quantity, such as a state in some defined coordinate system or a state as a vector in Hilbert space of QFT, so I preferred to only say “field”.
It's just like, if talking about an electron, I could say that what's real is “an electron with momentum \vec{p} with respect that coordinate system”, but I'd generally prefer (for brevity if you want) to say that what is real is only the electron.

tom.stoer said:
Anyway, the concept of reality becomes even more veiled and vague ... or even void

I'd say the exact opposite, but this deserves a separate thread.

I have my own definition of reality, that in my opinion is very solid (although dynamic), but I don't think that talking about this could be useful in this discussion.

Ilm
 
  • #17
tom.stoer said:
It was disturbing to lose the concept of "reality of values of attributes of particles" in QM (you cannot assign attributes like spin, etc. to a particle before this atrtribute of the particle has been measured). But in QM there was no problem with the particle itself.[/itex]

I don't agree, I think there is some problem in the usual QFT definition of particles... :smile:

tom.stoer said:
Now we do not only lose the concept of "reality of values of attributes of particles" but the concept of "reality of particles".

I think this *is* disturbing (when thinking about reality; if you stick to positivism there is no such problem ;-)

Then simply take fields as fundamental entities, as I suggested before.

If you do so particles are only “attributes of fields” and you don't lose the “reality of fields” but only the “reality of values of attributes of fields”. :-p

Ilm
 
  • #18
The problem is that you don't detect fields but particles.

The concept of fields in quantum field theory is a mathematical model; you cannot say whether it's real b/c it never has been observed. Particles i.e. "ticks in detectors" have been observed ;-)
 
  • #19
tom.stoer said:
The problem is that you don't detect fields but particles.

The concept of fields in quantum field theory is a mathematical model; you cannot say whether it's real b/c it never has been observed. Particles i.e. "ticks in detectors" have been observed ;-)

I'm sorry but I don't agree again ;-)

What we see are not, strictly speaking, particles. We see as you said “ticks in detectors”.

Ticks are caused by some property of the object observed, such as charge, momentum, position, etc.

Are these property of a field or of a particle? The ticks do not answer these question, as an answer depends on the physical theory you are using to interpret the ticks.

To my opinion QFT is not a theory of particles, is a theory of fields. Particles are only something we use to describe fields configuration, we could predict the same ticks in detectors without even naming particles.

So, in my opinion, particle content of a system has to be regarded exactly as the momentum of that system, i.e. as some label (that depends on coordinates used) describing the system configuration (within our theory).

Ilm
 
  • #20
This discussion seems to suffer from a certain mixing up of "the map and the territory" kind of problem.
Since I think the OP concern about reality regarding the Unruh effect goes beyond that trivial confusion I'll try to distinguish it so that physics and philosophy don't get mixed up.
A useful assumption (usually a tacit one) in science is that there is just one reality but as observers we only get access to it thru a particular POV, so that as long as we agree about how to go from one POV to another everything should be fine.
This is different from the kind of explanations given by Ilmrak that are rather in the realm of the distinction between the unique reality beneath the multiple models and the models themselves.
So I agree with Tom that the Unruh effect is disturbing for the commonly used in science unique reality assumption due to the lack of the adequate mathematical tools to connect different POV's.
This doesn't happen neither in the SR relativity of simultaneity nor in flat QM-QFT.
 
  • #21
TrickyDicky said:
[...] So I agree with Tom that the Unruh effect is disturbing for the commonly used in science unique reality assumption due to the lack of the adequate mathematical tools to connect different POV's. [...]

I thought that in the Unruh effect we do know exactly how to connect vacua relative to different points of view... Am I missing something? :confused:

Ilm
 
  • #22
Ilmrak said:
I thought that in the Unruh effect we do know exactly how to connect vacua relative to different points of view... Am I missing something? :confused:

Ilm
You are missing the basic question if there is a unique underlying reality. To my little daughter it makes not so much difference if there is a Mars or a Snickers bar. What really matters is whether there is at least one chocolate bar. Believe me or not, she will not be convinced when you are trying to explain that there is an accelerated observer which can detect (and eat) a Snickers bar.

We do not face something like that in SR, GR, QM ant even in QFT (in flat space)!
 
  • #23
tom.stoer said:
In contrast to other oberver dependent effects this is not just a different interpretation of one frame-independent reality but seems to be a challange for physical reality at all.
IMO, the biggest challenge to "physical reality" is defining what we mean by the term, particularly from an experimental/scientific perspective. Once we have a testable definition then we can apply it and see, until then we are just discussing philosophy.

Do you have a proposal for a "physical reality" test?
 
  • #24
An interesting question Tom. I think I am tending towards Ilmrak's view. The fields are the basic entities. If an excitation of that field can have have a property that ranges over some values, which is frame dependant (e.g. momentum), why can that not be zero?
 
  • #25
tom.stoer said:
You are missing the basic question if there is a unique underlying reality. To my little daughter it makes not so much difference if there is a Mars or a Snickers bar. What really matters is whether there is at least one chocolate bar. Believe me or not, she will not be convinced when you are trying to explain that there is an accelerated observer which can detect (and eat) a Snickers bar.

We do not face something like that in SR, GR, QM ant even in QFT (in flat space)!

I'm sorry but I can't still understand why the unique underlying reality has to show/have the same defined number of particles in all frames of reference.

I mean, take relativistic redshift. If you have 1 red photon and 0 blue photon in some coordinates, in some other coordinates you have 0 red and 1 blue photon. The particle content change for the two points of view.

How Unruh effect rise more doubts than this on the reality of a particle?

Proceeding with you metaphor, why should she believe that the same chocolate bar that has peanuts for her but hasn't for an accelerating observer?
Moreover, maybe she is allergic to peanuts so that having a Snickers is equivalent to having nothing for her...

Ilm
 
  • #26
tom.stoer said:
You are missing the basic question if there is a unique underlying reality.

But that cannot IMO be formulated as a scientific question, but as I said it is rather a working assumption to apply the scientific method, whether or not one is aware of it. Otherwise it is not possible to trust any result, even the unassuming "shut up and calculate" no-philosophy of science uses that consistency requirement as a tacit assumption.
 
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  • #27
Ilmrak said:
I thought that in the Unruh effect we do know exactly how to connect vacua relative to different points of view... Am I missing something? :confused:

Ilm

As commented, there is a mathematical, and therefore physical disconnect between the accelerated observers and the other observers.
 
  • #28
As a layman this situation reminds me a bit of the situation back when Einstein came up with SR. So, as a layman, I'll ask a rather silly question: what if the particle count is real, and the Unruh effect is wrong, at least w.r.t. particle counts?

What modifications would have to be made in this case?
 
  • #29
We need Naive realism for the validity of biology, history, geography, etc. sciences as true descriptions of the world(otherwise we run into logical contradictions and inconsistencies). Can we return to naive realism? Ever?
 
  • #30
@Maui: we can't! We have something like "veiled reality" (Bernard d’Espagnat) which is already a strange issue, but the Unruh effects adds additional problems regarding "reality". Of course one could believe in "structural realism" using field operators and states but that has nothing to do with realism (in the naive sense) which requires at least some "correspondence" between "reality" and "perception". If you give up these concept you should no longer call it "realism" or "reality".

@Ilmrak: I see two problems
a) with one red and one blue photon we still can agree on the total number of photons, i.e. on the number of ticks registered by the detector; with the Unruh effect the number of ticks changes depending on the observer (which is logically no problem for each single tick b/c for the two observers we need to detectors and one single particle is registered in one and only one detector)
b) your position seems to be closed to positivsm, therefore you don't really care about my problem; or you tend to call something "real" b/c you use it to do calculations (like a field operator); I would call this "structural realism" and it's logically consistent, of course
 
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  • #31
TrickyDicky said:
As commented, there is a mathematical, and therefore physical disconnect between the accelerated observers and the other observers.

Sorry I still don't understand this.
The connection between the accelerated observer and the inertial one is continuous...
Could you please explain another time what are you meaning? :confused:

tom.stoer said:
@Maui: we can't! We have something like "veiled reality" (Bernard d’Espagnat) which is already a strange thing, but the Unruh effects adds additional problems. Of course one could believe in a structural realism using field operators and states but that has nothing to do with realism (in the naive sense) which requires at least some "similarities" between "reality" and "perception". If you give up these concept you should no longer call it "realism" or "reality".

@Ilmrak: I see two problems
a) with one red and one blue photon we still can agree on the total number of photons, i.e. on the number of ticks registered by the detector; with the Unruh effect the number of ticks changes
b) your position seems to be closed to positivism, therefore you don't really care about my problem; or you tend to call something "real" b/c you use it to do calculations (like a field operator); this I would call "structural realism" and it's logically consistent

How Unruh effect rise more doubts than this on the reality of a particle?

a) If your detector is only sensible to red photons then in one frame it ticks but not in the other.
I agree this is a bit different from what happens in the Unruh effect, but what I'm saying is that using a detector in an inertial frame or in presence of a gravitational field is as setting two different experiments and so seems natural to have two different results (as long as the laws that describes such results are the same in the two frames).
b) Yes, maybe what you call “structural realism” could be close to my position.

Anyway, I still have some difficulties in understanding exactly what's the point on which we are debating :-)

Sorry if I insist on this, but could you explain exactly in what is the Unruh effect more challenging then the fact that in GR the energy contained in some fixed region of space depends on the coordinate system used?
As I understand it there are not much interpretation differences besides the exchange particle\leftrightarrowenergy, and I don't get why particles are "more real" then energy. :smile:

DaleSpam said:
IMO, the biggest challenge to "physical reality" is defining what we mean by the term, particularly from an experimental/scientific perspective. Once we have a testable definition then we can apply it and see, until then we are just discussing philosophy.

Do you have a proposal for a "physical reality" test?

Maybe you're right and we should debate on what the “physical reality” is to resolve this...

Ilm
 
  • #33
Physics Monkey said:
Along the lines of what Vanadium 50 said earlier, you will probably be interested in looking at this paper: http://prd.aps.org/abstract/PRD/v29/i6/p1047_1
Great, thanks. Yes, it seems that there is in fact no logical inconsistency and that even physical interpretations are OK. Let me think about it for a while ...
 
  • #34
tom.stoer said:
Sorry to say that but reality in the philosophical sense is never about an "observer's reality"; refer e.g. to Wikipedia: "... reality includes everything that is and has been, whether or not it is observable or comprehensible". What you are talking about are perceptions.

[...] there is - by definition - only one reality.
For the record, I reject the notion of one single absolute total reality -- I find the notion insufficiently supported by experiment. Rather, I prefer the Rovellian argument that different noninertial observers can give inequivalent, nonisomorphic accounts of their perceived realities, as each measures it, due to horizons, etc.

In reality there should be one particle (one event that a particle is at a certain location) or there should be no particle. And this is independent from any observer.
No. There may indeed be a Mars bar in the accessible event set of one observer, but not the other, if a Rindler horizon intervenes.

[@Ilmrak: I don't think you're missing anything. Your explanations seem fine to me.]
 
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  • #35
strangerep said:
For the record, I reject the notion of one single absolute total reality -- I find the notion insufficiently supported by experiment. Rather, I prefer the Rovellian argument that different noninertial observers can give inequivalent, nonisomorphic accounts of their perceived realities, as each measures it, due to horizons, etc.
(sometimes) even philosophers use strict definitions - and ''perceived reality" misses the essential point. You have observer dependent perceptions (obviously) and you may have or believe in one single underlying observer-independent (!) reality. Observer dependent realities or perceived realities are a contradictio in eo ipso. You should call them simply perceptions or phenomena, not reality. Perhaps these philosophical terms may not map directly to our mathematical structures we use in QFT, but we should be clear about them.

strangerep said:
No. There may indeed be a Mars bar in the accessible event set of one observer, but not the other, if a Rindler horizon intervenes.
This is about perceptions and physical predictions; that's fine and nothing is missed - except for a definition of reality. I would not translate "accessable event set" as reality.

The basic question is whether the concept "event" or "one particle" can be an element of an underlying reality, or if it is an element of oberver dependent perceptions. If the latter one is assumed, what is the underlying reality? or do we want to give it up completely and stick to positivism? Does the particle exist w/o any observation or detection? In QM the answer is either "yes" (for all observers) or "no" (for all observers) and we only need to consider different perceptions (momentum, color, ...) of the same particle. In QFT this fades away and it seems that we cannot say that the particle exists independent from any observation. Not even the concept of "average number of particles in a given volume" cannot be used as an element of reality w/o contradiction.
 
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  • #36
Tom.stoer, have you seen my post #8? I would like to see your comments on it.
 
  • #37
Demystifier said:
Tom.stoer, it is possible to retain objective status of particles in the Unruh effect, provided that a preferred time exists as in Horava gravity. See
http://xxx.lanl.gov/abs/0904.3412

Very interesting aticle, I missed that post.
I'm a bit sceptical cause I'd really like to have Lorentz invariance at small distances, but I'll have to read more about this.

Ilm
 
  • #38
Sorry to pop in a bit late, but I would like to give my point of view.

How can an event be observer dependent without any underlaying reality?

In SR this seems impossible.Because how can the event -f.ex. a lightning hitting a tree'- only be observer dependent without any underlaying reality of a tree and a lightning? That's seems impossible to me. I do not see how a tree can be 'created' purely and only by our perception, measuring machines etc. That looks more like dreaming (a PF thread was closed because of this dreaming scenario). If you want to stick to that, you are positivist/solipsist.

In QM different but same story. Do we fabricate/measure particles out of nothing, a 'creatio ex nihilo'? Maybe there are no particles out there, but at least 'something' (call it a field if you like) must be out there to help 'make' the particles.

If the simple fact of observing creates a reality, then we really have to go into philosophy.

Unless you are a positivist/solipsist we have to accept that physics forces us to believe there is an observer independend reality. In QM this might be a non-observable reality. In SR it is an observable reality, through our different 3D space cuts (relativity of simultaneity) through 4D Spacetime. But positivists/solipsists will of course call all this only mathematical working models in their dream state of being :-)
 
  • #39
Vandam, I agree with you and that was the point of my post about science requiring the "unique underlying reality" to be logically consistent.
Apparently this is not well understood by most here, it looks like the solipsist school of thought is more fashionable nowadays.
 
  • #40
This thread has been re-opened.

Please ensure that your post has actual physics content, and it is not JUST a philosophical discussion devoid of physics (i.e. it is based on clear, unadulterated physics theory and/or experiment). A point made simply based on a matter of "tastes" will result in this thread suffering from the same fate.

Zz.
 
  • #41
It would be important to make the distinction between the Unruh effect proper and Unruh radiation, the latter is not fully accepted by the physics community according to wikipedia.
The answer given in #2 applies to the former, however Tom's questions seemed to refer to Unruh radiation
.
 
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  • #42
I am not sure if I correctly understand the difference between Unruh effect and Unruh radiation. The Unruh effect means that an accelerating observer will se a thermal state. But what else but a "gas or particles" can this thermal state be?
 
  • #43
Vanadium 50 said:
what one observer characterizes as absorbtion, the other characterizes as emission.

Wikipedia entry:
"While the skeptics accept that an accelerating object thermalises at the Unruh temperature, they do not believe that this leads to the emission of photons, arguing that the emission and absorption rates of the accelerating particle are balanced."
 
  • #44
tom.stoer said:
The Unruh effect claims that a quantum state which can be defined as an "empty vacuum state" by an inertial observer will become a "thermal state containing particles" for an observer with constant acceleration a; the temperature observed is T ~ a.

In contrast to other oberver dependent effects this is not just a different interpretation of one frame-independent reality but seems to be a challange for physical reality at all. Let me explain why.

Suppose we are detecting particles in different references frames, i.e. with different detectors. Each time we are detecting a particle we agree that there is a particle, but we are not in agreement regarding its energy. We are not worried about this fact b/c we can use a Lorentz transformation to get the relation between energy and momentum.

For the Unruh effect it becomes much more disturbing b/c we cannot even agree whether there there is a particle or not. So it seems that we are no longer talking about one unique quantum state with frame dependent interpretations but that we have two truly different quantum states, two different "realities". There is not one event "a particle" with different interpretations like "energies E, E', E'', ...", but there are different realities some with an event "a particle", some with "no particle".

Suppose an accelerating observer and a goup of stationary observers at rest collect the information regarding "their quantum states" over a couple minutes. Once the accelerating observer passes a stationary one they make a simultaneous measurement whether there is a particle or not. After a while the obervers at rest will not have counted any particle, but the accelerating observer will have counted many. So they disagree on the fact "whether there are particles at all".

b/c every particle can be detected only once one could get rid of the problem via the idea that the particles detected by the accelerated observer cannot be detected by the obsevers at rest, so there is no logical contradiction. This is OK, but of course the accelerating observer "knows" that there are other particles that he could detect in principle, but that they escape from his detector by whatever reason. These particles are not detected by the observers at rest, not even in principle.

So the particles detected by the accelerated observer are not and cannot be detected by the observers at rest (b/c they can be detected only once). And the particles not detected by the accelerated observer are not and need not be detected by the observers at rest. So it really seems that there is no logical contradiction - but you may understand that when talking about "reality" one may be bothered by these ideas.

Any thoughts?
The following is a conjecture. I am speculating on the importance of the event horizon in the accelerated observers frame.
The observer in the accelerating frame vehicle sees an "event horizon" in the direction opposite the direction of the acceleration vector. The event horizon is analogous to a very big black hole. The observer in an inertial frame does not see this event horizon. However, he sees that light emitted from behind the accelerated observer vehicle can never catch up to the accelerated observer vehicle. I think that it is the event horizon that resolves the Unruh conundrum.
In order to emit Bremstrahlung radiation, there has to be a charged particle that is being accelerated. An observer traveling with this charged particle sees a stationary electric charge, and an event horizon.
The accelerated observer sees a sky emitting thermal radiation. In the eyes of the accelerated observer, the electric charge is an antennae for electromagnetic radiation. Some of the thermal radiation is absorbed by the electric charge antennae. All thermal radiation not absorbed by the antennae is swallowed by the event horizon that is a finite distance from the antennae. The energy swallowed by the event horizon is lost forever to both observers.
The inertial observer does not see the thermal photons as thermal photons. He sees the thermal photons as virtual photons. In other words, the thermal distribution of photons in the accelerated frame is seen as a Lorentz invariant distribution of photons in the inertial frame. Because the Lorentz invariant distribution is a zero point radiation, it is not seen in the inertial frame. The Lorentz invariant distribution is sometimes called the virtual photons.
The photons that are absorbed by the "antennae" in the accelerated reference frame reappear as photons in the inertial reference frame. The gravitational gradient seen in the accelerated frame provides enough energy to the virtual photons to become real photons in the inertial frame.
Thus, the electric charge is an emitting antennae in the inertial frame. The accelerating electric charge emits Bremstrahlung radiation in the inertial frame.
Thus, one can look at it this way. A virtual photon falls down in the accelerating frame, acquiring enough energy to become a real photon. If it is absorbed by an electric charge, then it appears to the inertial observer as an emitted photon. If the virtual photon misses the electric charge, it is absorbed by the event horizon and never seen again by either observer.
 
  • #45
@Demystifier: regarding post #8

Demystifier said:
Tom.stoer, it is possible to retain objective status of particles in the Unruh effect, provided that a preferred time exists as in Horava gravity. See
http://xxx.lanl.gov/abs/0904.3412
This is a rather interesting attempt. However one should not overburden Horava gravity here. Isn't it possible to 'derive' a similar result simply by forbidding t-r-mixing coordinate transformations? That would mean that in any theory of gravity "similar" to GR, Horava, ... there is an objective notion of "vacuum" for an "equivalence class" of geometries related by "allowed transformations"?

The problem I see is the following: both Unruh and Hawking radiation are "global" effects; they rely on a global definition of space-time (used to define the frequencies and creation / annihilation operators) and they rely on (asymptotic) plane wave or plane-wave-like states. But the observation of an observer is alaways a local one!

In addition the relation between an asymptotic observer (observing Hawking radiation) and a free-falling observer crossing the event horizon must not be restricted by excluding certain transformations. I mean the fact that the observer is in free fall is a physical statement. So it is irrelevant for the observers whether there is a transformation relating an asymptotic observer and a free-falling observer. The observers are observing something and this 'something' is of course not affected by such a transformation.

My conclusion is therefore a bit different: ruling out certain transformations in Horava gravity seems to indicate that a definition of vacua using global rules is in conflict with GR (and similar theories) excluding global entities (like energy as a volume integral). Therefore the idea should be to get rid of a definition of vacua relying on such global entities (as has been done for EHs in the meantime which can be characterized locally w/o referring to lightlike infinity).

---------

Let me ask the following question again:

tom.stoer said:
I am not sure if I correctly understand the difference between Unruh effect and Unruh radiation. The Unruh effect means that an accelerating observer will see a thermal state. But what else but a "gas or particles" can this thermal state be?
 
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  • #46
tom.stoer said:
The problem I see is the following: both Unruh and Hawking radiation are "global" effects; they rely on a global definition of space-time (used to define the frequencies and creation / annihilation operators) and they rely on (asymptotic) plane wave or plane-wave-like states. But the observation of an observer is alaways a local one!

My conclusion is therefore a bit different: ruling out certain transformations in Horava gravity seems to indicate that a definition of vacua using global rules is in conflict with GR (and similar theories) excluding global entities (like energy as a volume integral). Therefore the idea should be to get rid of a definition of vacua relying on such global entities (as has been done for EHs in the meantime which can be characterized locally w/o referring to lightlike infinity).
Your idea that particles should be defined locally is developed in more detail here:
http://xxx.lanl.gov/abs/gr-qc/0409054 [Class.Quant.Grav.26:025002,2009]
 

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