Where Does the Energy of Redshifted Light Go?

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Redshifted light loses energy as it travels through the expanding universe, raising questions about where that energy goes. Energy is not necessarily conserved in General Relativity, which allows for scenarios where energy loss occurs without violating conservation laws. The discussion highlights that while photons lose energy due to redshift, this can be understood through the conservation of the stress-energy tensor in a comoving volume. Additionally, the possibility of thermalization of light in different media is explored, with examples like the Sunyaev-Zel'dovich effect illustrating how low-frequency light can gain energy. Ultimately, the isotropy of the Cosmic Microwave Background (CMB) and its anisotropies support the hot dense early universe model, ruling out alternative theories that do not align with observed data.
  • #31
JuanCasado said:
Why not?

Cheers

Basically, almost any process removing energy from photons is going to distort the spectrum, unless there is a very special relationship between the energy of photons and the energy they loose. The real onus is on anyone wanting to demonstrate some physical process that somehow could remove just the right amount of energy from photons to maintain a blackbody.

Photons in a blackbody spectrum are distributed over the whole spectrum. If thermalized with matter, the colder photons will tend to heat up, and the hotter ones cool down, so that the spectrum is bound to be distorted.

This is observed... through in reverse. Background radiation is extremely cold, and so in its interactions with matter the tendency is for the photons to pick up energy from the interaction. It's called the Sunyaev-Zel'dovich effect, in which interactions with hot matter give a blueshift. This distorts the spectrum away from a blackbody, as we should expect. The same thing would occur in reverse with compton cooling of radiation, which is why we cannot get a cold blackbody spectrum by cooling hot radiation using interactions with cold matter.

Cheers -- Sylas
 
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  • #32
  • #33
time dilation resolves the apparent energy loss - lower energy photons are received over a longer period of time. the result is the same. how hard is that to understand?
 
  • #34
Chronos said:
time dilation resolves the apparent energy loss - lower energy photons are received over a longer period of time. the result is the same. how hard is that to understand?
Well, as I said, there are multiple ways to look at it. If we consider, for instance, the photons within a comoving volume, the number density will stay the same with the expansion, but their wavelength will get larger, resulting in a lower energy in an expanded volume than before expansion.
 
  • #35
from the perspective of any given observer, the redshifted photons will persist over a long periond of time. the total energy will be preserved.
 
  • #36
Chronos said:
from the perspective of any given observer, the redshifted photons will persist over a long periond of time. the total energy will be preserved.
That's just not the case though. Not unless you use the Hamiltonian formalism which includes gravitational potential energy, that is. Just a simple example shows this is so: the energy density in photons now is non-zero (though pretty small compared to matter). Fast forward to the asymptotic future assuming the universe continues to expand, and the total energy in photons any volume you pick will be zero.
 
  • #37
Well, I was not referring to hot plasma among galaxies within a cluster, but to very cold matter in the voids among the clusters...
 
  • #38
JuanCasado said:
Well, I was not referring to hot plasma among galaxies within a cluster, but to very cold matter in the voids among the clusters...

I understand that; and specifically allowed for it in my explanation for why it can't explain the CBR. Repeating what I said before:

sylas said:
... The same thing would occur in reverse with compton cooling of radiation, which is why we cannot get a cold blackbody spectrum by cooling hot radiation using interactions with cold matter.

In interactions with matter, a blackbody spectrum is not preserved. The CMB has a fantastically accurate blackbody spectrum. Therefore the CBR is not some originally hotter radiation that has been cooled (redshifted) by comptomization -- which is what you are asking about.

It is all the same process; energy transfer between radiation and matter, when there is a temperature difference. It's known and studied. The process of "compton cooling" and "compton heating" are the same physical process, and it does distort a blackbody spectrum. You are proposing "compton heating" (which means hotter matter and a cooler radiation temperature). It's a neat idea, but it can't work for explaining the CBR.

Cheers -- Sylas
 
  • #39
I perceive a misunderstanding of general relativity. Do you have any particular math in mind, Chalnoth? I do.
 
  • #40
JuanCasado said:
Well, I was not referring to hot plasma among galaxies within a cluster, but to very cold matter in the voids among the clusters...
But why would you think that matter is very cold? Certainly it's not as absurdly hot as the matter within clusters, as that matter has been heated up by falling into the large gravitational potential wells. But it still tends to be ionized due to starlight.
 
  • #41
Chronos said:
I perceive a misunderstanding of general relativity. Do you have any particular math in mind, Chalnoth? I do.
You do realize that energy is not always conserved in General Relativity, right?
 
  • #42
JuanCasado said:
Good. So, could CMB photons be (conversely) red shifted, i.e. "cooled down", due to interactions with very cold intergalactic media?
Only if that medium were colder than the CMB, which isn't the case.
 
  • #43
Chalnoth said:
Only if that medium were colder than the CMB, which isn't the case.

What is the temperature of that medium?
 
  • #44
sylas said:
In interactions with matter, a blackbody spectrum is not preserved. The CMB has a fantastically accurate blackbody spectrum. Therefore the CBR is not some originally hotter radiation that has been cooled (redshifted) by comptomization -- which is what you are asking about.

It is all the same process; energy transfer between radiation and matter, when there is a temperature difference. It's known and studied. The process of "compton cooling" and "compton heating" are the same physical process, and it does distort a blackbody spectrum. You are proposing "compton heating" (which means hotter matter and a cooler radiation temperature). It's a neat idea, but it can't work for explaining the CBR.

Cheers -- Sylas

Thanks for the details. In fact I was proposing cooler matter and hotter radiation. Any references supporting the "distortion" you mention?
 
  • #45
JuanCasado said:
Thanks for the details. In fact I was proposing cooler matter and hotter radiation. Any references supporting the "distortion" you mention?

What I mean is that you are proposing radiation that gets colder, and matter that gets hotter, as a result of the interaction.

I've already given you the key terms to look for, though unfortunately they are only for the case where cold radiation is made hotter. Here's a page on the Sunyaev-Zel'dovich Effect which includes a diagram illustrating the distortion for this case. Here's the diagram:
fig1.jpg

The rightward shift is the heating effect on the radiation; the distortion is the small change in shape you can see. It diverges from the blackbody spectrum.

What you are proposing is the same physical process, but in reverse, with cold matter. And I don't know of a corresponding diagram, nor even of a case where it is measured. It may be that at such cold temperatures the effect becomes less, well, effective. I'm not sure. It would have to be very cold indeed, because the CMBR is only about 2.7 degrees above absolute zero.

Cheers -- Sylas
 
  • #46
sylas said:
What I mean is that you are proposing radiation that gets colder, and matter that gets hotter, as a result of the interaction.

I've already given you the key terms to look for, though unfortunately they are only for the case where cold radiation is made hotter. Here's a page on the Sunyaev-Zel'dovich Effect which includes a diagram illustrating the distortion for this case. Here's the diagram:
fig1.jpg

The rightward shift is the heating effect on the radiation; the distortion is the small change in shape you can see. It diverges from the blackbody spectrum.

What you are proposing is the same physical process, but in reverse, with cold matter. And I don't know of a corresponding diagram, nor even of a case where it is measured. It may be that at such cold temperatures the effect becomes less, well, effective. I'm not sure. It would have to be very cold indeed, because the CMBR is only about 2.7 degrees above absolute zero.

Cheers -- Sylas

Do you realize that in the figure quoted "the SZE distortion shown is for a fictional cluster 1000 times more massive than a typical massive galaxy cluster", so that the effect I am proposing will be practically null and would yield an spectrum undiscernible from a blackbody spectrum?
Regards
 
  • #47
JuanCasado said:
Do you realize that in the figure quoted "the SZE distortion shown is for a fictional cluster 1000 times more massive than a typical massive galaxy cluster", so that the effect I am proposing will be practically null and would yield an spectrum undiscernible from a blackbody spectrum?
Regards

Of course I do realize the SZE effect is small.

But no, the effect you are proposing is NOT nearly null. You are proposing a very large effect indeed! That's another tremendous physical difficulty with invoking matter interactions. The problem is to explain a very cool background radiation, showing the spectrum of a thermodynamic blackbody at a fantastically cold 2.7 degrees above absolute zero.

The conventional explanation is that cosmic microwave background radiation is from a source that is at about 3000K; but redshifted by a factor of about 1100 from the cosmological redshift -- the same process that gives a redshift to distant galaxies. This works, because redshift from an increase in the scale factor does preserve a Planck spectrum. This can therefore account for the large shifts needed to give a very cold CMBR.

You have suggested an alternative; that it comes from some hot source, and has been cooled, not by processes connected with velocity or gravitation or scale factor, but by interactions with matter. The effect has to be very large, because the radiation is very cold.

Interactions with matter will distort a Planck spectrum. If there is any significant level of cooling in the radiation, there will necessarily be a correspondingly significant distortion of the spectrum.

You've actually hit here upon another reason to think interactions with matter won't work. As you note, interactions with matter tend to have a very small effect indeed. That only makes it harder to find sufficient time and matter to cool hot radiation down by the large amounts you require. In fact, this might be a better way to help you see why interactions with matter are physically not able to account for the CMBR.

Cheers -- Sylas
 
  • #48
JuanCasado said:
What is the temperature of that medium?
It's not well-described by a single temperature, as it's not in thermal equilibrium (as I said, it's ionized by stars).

Oh, and by the way, the result of this cooling wouldn't be a thermal spectrum either. The CMB has an almost perfect blackbody spectrum.
 

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