The Definition of Redshift for Photons

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Discussion Overview

The discussion revolves around the definition of redshift for photons, particularly in the context of cosmological redshift within Friedmann-Robertson-Walker (FRW) spacetime. Participants explore the relationship between energy, proper time, and the scale factor in cosmology, as well as the implications of using different forms of energy expressions.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant questions whether the correct form for associating a timelike Killing vector field (KVF) with energy should be ##\dot{t}^2## or ##\dot{t}##, suggesting a preference for the former based on classical analogies.
  • Another participant clarifies that the energy measured by an observer is ##m dt / d\tau##, where ##m## is the invariant mass, and distinguishes this from energy associated with a timelike KVF, which involves the metric tensor and 4-momentum.
  • There is a discussion about the proper times of observers and the light ray, with one participant noting that the light ray does not have a proper time since its worldline is null.
  • Participants explore the implications of the scale factor in FRW spacetime on redshift, stating that the wavelength increases if ##a(t_2) > a(t_1)##.
  • One participant expresses confusion about the relationship between energy and wavelength, questioning how to deduce energy changes from wavelength variations.
  • Another participant emphasizes that the energy formula ##E=mdt/d\tau## applies to timelike objects and seeks clarification on its application in the context of the discussion.
  • There is a suggestion that a change in frequency, related to wavelength, causes a change in energy, linking ##E=\hbar\nu## and ##\nu=c/\lambda##.

Areas of Agreement / Disagreement

Participants exhibit a mix of agreement and disagreement, particularly regarding the application of energy formulas and the relevance of timelike KVFs in the context of FRW spacetime. The discussion remains unresolved on several points, particularly concerning the proper interpretation of energy in relation to redshift.

Contextual Notes

There are limitations in the discussion regarding the assumptions made about the observers and the definitions of terms used, particularly concerning the invariant mass and the nature of the energy being discussed. The relevance of the timelike KVF in FRW spacetime is also contested.

  • #31
@binbagsss : It is hard to guess what exactly you are asking, as you can tell from all the posts above. But you can find in Wald's book the derivation of the redshift for the Schwarzschild solution using the time-like Killing field. You can also find the trick how to do that in the FRWL space-time although there is no time-like Killing field.
 
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  • #32
binbagsss said:
I am really asking what is the definition of red-shift.

The shift in frequency (or wavelength) of spectral lines observed in light from distant objects, as compared with the frequency (or wavelength) of those same lines in a lab.

binbagsss said:
red- shift is defined as the difference in time between two light rays as observed by two different observers.

Is it? Look at the definition I just gave above. You might be confusing how redshift is defined with how it is calculated in a particular model (more precisely, how a prediction of what redshift would be observed in a particular observation, is calculated in a particular model).
 
  • #33
PeterDonis said:
The shift in frequency (or wavelength) of spectral lines observed in light from distant objects, as compared with the frequency (or wavelength) of those same lines in a lab.
Is it? Look at the definition I just gave above. You might be confusing how redshift is defined with how it is calculated in a particular model (more precisely, how a prediction of what redshift would be observed in a particular observation, is calculated in a particular model).

PeterDonis said:
The shift in frequency (or wavelength) of spectral lines observed in light from distant objects, as compared with the frequency (or wavelength) of those same lines in a lab.
Is it? Look at the definition I just gave above. You might be confusing how redshift is defined with how it is calculated in a particular model (more precisely, how a prediction of what redshift would be observed in a particular observation, is calculated in a particular model).

Ok, so and how does the method for computing the predictions differ for instance, in the frw model and schwarzschild metric - how do you decide which method for a particular model is going to give you the prediction of that observation
 
  • #34
martinbn said:
@binbagsss : It is hard to guess what exactly you are asking, as you can tell from all the posts above. But you can find in Wald's book the derivation of the redshift for the Schwarzschild solution using the time-like Killing field. You can also find the trick how to do that in the FRWL space-time although there is no time-like Killing field.

Yes I have seen this in Carroll via a killing vector tensor, instead
 
  • #35
binbagsss said:
how does the method for computing the predictions differ for instance, in the frw model and schwarzschild metric

It doesn't have to. You can use the same method for both. But the method that works for both does not involve the proper time of either the emitter or the receiver. It's the method you used in your calculation earlier in the thread, which I discussed in post #21; you can do that same kind of calculation in Schwarzschild spacetime, but of course the specific expression for the metric is different, so you will get a different final expression for the redshift--the one you are used to seeing for Schwarzschild spacetime. Try it!
 
  • #36
PeterDonis said:
. The redshift of the photon, as you will see if you do this analysis, then turns out to be, as I said before, the ratio of the scale factor at reception to the scale factor at emission--more precisely, this ratio is equal to ##1 + z##, where ##z## is the redshift.

In previous posts I was trying to establish the definition of red shift, (well the predicted redshift not the lab spectral line observed measurement) and there was no such direct response, other than that of observation. Well if we determine ##k## by the method you described, and ##k## is such that the photon is null, then that is something we are comparing - you used the term red-shift twice above. Somehow it is plausible to immediately state that the 'red shift if the photon' is given by comparing these frequencies, but then you use redshift to refer to ##z## - the only mysterious definition I was pointed to. The important parameter was what I was after, so it's ##k## ? It's so obvious that you can compare frequencies to give the red shift if the photon that you don't even explain this, yet all my questions where pointed toward ##z## ...
 
  • #37
binbagsss said:
In previous posts I was trying to establish the definition of red shift, (well the predicted redshift not the lab spectral line observed measurement) and there was no such direct response, other than that of observation.

Sure there was; I gave you the definition of redshift in post #32.

binbagsss said:
if we determine ##k## by the method you described, and ##k## is such that the photon is null

I don't know what you mean here; ##k## itself doesn't tell anything about whether the photon's worldline is timelike or null; you have to already know that the photon's worldline is null in order to determine ##k## by the method I described.

I've already said once that if you do the actual math, it will make all this a lot clearer. Have you done the actual math?

binbagsss said:
Somehow it is plausible to immediately state that the 'red shift if the photon' is given by comparing these frequencies, but then you use redshift to refer to z

I don't understand what your issue is. If you want the precise mathematical definition, here it is: we observe a particular spectral line in the lab to have a wavelength ##\lambda_{\text{lab}}##. We observe the same spectral line in light from a distant object to have a wavelength ##\lambda_{\text{obs}}##. Then

$$
1 + z = \frac{\lambda_{\text{obs}}}{\lambda_{\text{lab}}}
$$

If you want it in terms of frequencies instead, then we have the lab frequency ##\nu_{\text{lab}}## and the frequency observed from the distant object ##\nu_{\text{obs}}##, and then

$$
1 + z = \frac{\nu_{\text{lab}}}{\nu_{\text{obs}}}
$$

You can find these definitions in any textbook or in many places online; most of them will call ##\nu_{\text{lab}}## or ##\lambda_{\text{lab}}## the "emitted" frequency or wavelength, because we assume that the frequency/wavelength we observe in the lab will be the same as the frequency/wavelength emitted by the distant object (because the same substances should emit the same frequencies/wavelengths anywhere, since the physical laws governing emission are the same).

Is this what you were looking for? If not, what are you looking for?
 

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