CMBR anisotropy and cosmic abundances

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In summary, CMBR anisotropy refers to the slight variations in the temperature of the cosmic microwave background radiation across the sky. These variations provide valuable insights into the distribution of matter and energy in the early universe. By studying the anisotropy of CMBR, scientists can determine the abundance of different elements in the universe, such as hydrogen, helium, and lithium. This information helps us understand the processes that took place during the Big Bang and the evolution of the universe.
  • #1
Adrian59
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What is (are) the original paper(s) relating to the interpretation of the CMBR anisotropy in setting the cosmic abundances? I did pose the same question last year but it got lost in another thread. I had found papers by Hu and Dodelson from 2002, Hu and white from 1996 and Seljak from 1994 as well as a recent review by Tojerio 2006. More recently I have read Hu & Sugiyama (1995) paper. A clear technical answer appears to elude me for the mechanism of the relative heights of the peaks as evidence for the cosmic abundances of baryonic matter, dark matter and dark energy.
 
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  • #2
Cosmic abundances? You mean cosmic light element abundances? Or something else?
 
  • #3
kimbyd said:
Cosmic abundances? You mean cosmic light element abundances? Or something else?

No, I mean the ratios of dark energy 68%, dark matter 27%, baryonic matter 5% or something close to these since different references can differ slightly with these values but I think the ones I have quoted are to the nearest 1% the currently excepted values.
 
  • #4
I don't think estimation of these cosmological parameters was really possible until the WMAP satellite's first data release, so that would make this paper the first publication of somewhat-precise measurements of these values:
https://arxiv.org/abs/astro-ph/0302209

But are you looking for something else? As in, are you more interested in the theoretical underpinnings of how these cosmological parameters impact the CMB data? Are you more interested in the data processing that extracts information from the CMB (e.g. determining the power spectrum or determining cosmological parameters from the power spectrum)?
 
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  • #5
kimbyd said:
I don't think estimation of these cosmological parameters was really possible until the WMAP satellite's first data release, so that would make this paper the first publication of somewhat-precise measurements of these values:
https://arxiv.org/abs/astro-ph/0302209

But are you looking for something else? As in, are you more interested in the theoretical underpinnings of how these cosmological parameters impact the CMB data? Are you more interested in the data processing that extracts information from the CMB (e.g. determining the power spectrum or determining cosmological parameters from the power spectrum)?

Probably the latter but I will try the reference first; thanks for your help.
 
  • #6
Adrian59 said:
Probably the latter but I will try the reference first; thanks for your help.
Let me know! There's a lot of rich history involved in CMB science, most of it since 1990.
 
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  • #7
kimbyd said:
Let me know! There's a lot of rich history involved in CMB science, most of it since 1990.

Thanks. I have now read the reference you embedded. As suggested above I was looking more for as you said
kimbyd said:
in the data processing that extracts information from the CMB … determining cosmological parameters from the power spectrum)
.

I still find this paper does a similar slight of hand trick as the other papers I have read, in that results are quoted (as in table 1) without really showing how they were calculated. One often sees interactive graphics that show the CMBR isotropy change as you alter the ratios, but no idea of the algorithm behind the graphic.
 
  • #8
Adrian59 said:
I still find this paper does a similar slight of hand trick as the other papers I have read, in that results are quoted (as in table 1) without really showing how they were calculated. One often sees interactive graphics that show the CMBR isotropy change as you alter the ratios, but no idea of the algorithm behind the graphic.
Are you talking about the power spectrum of the CMB? These might be the videos you're referring to?
http://space.mit.edu/home/tegmark/cmb/movies.html

If so, Max Tegmark has a number of other resources on CMB data analysis. A lot of the info is a bit old, but still relevant. For the power spectrum itself, the relationship between cosmological parameters and the CMB is computed by simulating the behavior of the early universe using approximations which make the simulations tractable.

This paper describes the first algorithm which was used for rapid computation of the expected CMB power spectrum given a set of model parameters:
http://xxx.lanl.gov/abs/astro-ph/9603033

Today's computations haven't changed all that much from the above algorithm.
 
  • #9
Adrian59 said:
I still find this paper does a similar slight of hand trick as the other papers I have read, in that results are quoted (as in table 1) without really showing how they were calculated. One often sees interactive graphics that show the CMBR isotropy change as you alter the ratios, but no idea of the algorithm behind the graphic.

No sleight of hand. The paper states

We begin by outlining our methodology (§2). Verde et al. (2003) describes the details of the approach used here to compare theoretical predictions of cosmological models to data.

In other words, a brief outline for experts is given is section 2 "BAYESIAN ANALYSIS OF COSMOLOGICAL DATA", and a a more detailed treatment, again for experts, is given in

https://arxiv.org/abs/astro-ph/0302218

An advanced but possibly more readable treatment is given in chapter 6 "Cosmological parameter estimation" from the book "The Cosmic Microwave Background" by Ruth Durrer.
 
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  • #10
Thanks everyone, it appears I have some more reading.
 
  • #11
kimbyd said:
Are you talking about the power spectrum of the CMB? These might be the videos you're referring to?
http://space.mit.edu/home/tegmark/cmb/movies.html

If so, Max Tegmark has a number of other resources on CMB data analysis. A lot of the info is a bit old, but still relevant. For the power spectrum itself, the relationship between cosmological parameters and the CMB is computed by simulating the behavior of the early universe using approximations which make the simulations tractable.

This paper describes the first algorithm which was used for rapid computation of the expected CMB power spectrum given a set of model parameters:
http://xxx.lanl.gov/abs/astro-ph/9603033

Today's computations haven't changed all that much from the above algorithm.

Your first link to Max Tegmark site shows something like what I meant though his graphic doesn't appear to allow a freeze frame to show exactly what the CMBR anisotropy would look like with a particular choice of parameters. I'm afraid the second linked site is currently unavailable.
 
  • #12
George Jones said:
No sleight of hand. The paper states
In other words, a brief outline for experts is given is section 2 "BAYESIAN ANALYSIS OF COSMOLOGICAL DATA", and a a more detailed treatment, again for experts, is given in

https://arxiv.org/abs/astro-ph/0302218

An advanced but possibly more readable treatment is given in chapter 6 "Cosmological parameter estimation" from the book "The Cosmic Microwave Background" by Ruth Durrer.

I have read the paper you provided a link to. It seems very much the same group of authors for the link previously given. I have to admit that I am yet to be totally convinced that dark matter is a feature of our universe. As yet I still feel a paper which clearly goes from direct observational data on the CMBR to evidence of dark matter is missing. There appears to be an assumption that dark matter exists before the analysis. For example in part 6. Lyman α Forest Data it says as I quote, 'The Lyman α forest traces the fluctuations in the neutral gas density along the line of sight to distant quasars. Since most of this absorption is produced by low density unshocked gas in the voids or in mildly overdense regions that are thought to be in ionization equilibrium, this gas is assumed to be an accurate tracer of the large-scale distribution of dark matter.' In other words there appears an implicit assumption that there is dark matter.
 
  • #13
Adrian59 said:
I have read the paper you provided a link to. It seems very much the same group of authors for the link previously given. I have to admit that I am yet to be totally convinced that dark matter is a feature of our universe. As yet I still feel a paper which clearly goes from direct observational data on the CMBR to evidence of dark matter is missing. There appears to be an assumption that dark matter exists before the analysis. For example in part 6. Lyman α Forest Data it says as I quote, 'The Lyman α forest traces the fluctuations in the neutral gas density along the line of sight to distant quasars. Since most of this absorption is produced by low density unshocked gas in the voids or in mildly overdense regions that are thought to be in ionization equilibrium, this gas is assumed to be an accurate tracer of the large-scale distribution of dark matter.' In other words there appears an implicit assumption that there is dark matter.
It is difficult to track through the whole thought process for why the CMB is such powerful evidence for dark matter, but it is all there. Max Tegmark's movies linked above provide a nice visual for how dark matter influences the CMB (basically, it changes the even/odd peak structure). And the Seljak and Zaldarriaga paper demonstrates how that link is calculated in practice (if you want to trace the calculations back, they also provide references for how dark matter was originally included).

Finally, if you're concerned about how dark matter is "assumed" from the start, bear in mind that if dark matter didn't exist, the above analysis procedure would measure its density to be zero. It doesn't.
 
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  • #14
kimbyd said:
It is difficult to track through the whole thought process for why the CMB is such powerful evidence for dark matter, but it is all there. Max Tegmark's movies linked above provide a nice visual for how dark matter influences the CMB (basically, it changes the even/odd peak structure). And the Seljak and Zaldarriaga paper demonstrates how that link is calculated in practice (if you want to trace the calculations back, they also provide references for how dark matter was originally included).

Finally, if you're concerned about how dark matter is "assumed" from the start, bear in mind that if dark matter didn't exist, the above analysis procedure would measure its density to be zero. It doesn't.

I believe, I have with your help finally tracked down what I would consider the main papers in interpretation of the CMBR anisotropy. The original Hu & Sugiyama (1995) paper gives a model to the CMBR anisotropies. Seljak & Zaldarriaga (1996) formulate an analytical technique using line of sight integration for analysing the data from the CMBR probes. Then from the WMAP results Verde et al in 2003 show how the data is analysed using, first Baye’s theorem and then Markov chains with a Monte Carlo stimulation. Finally, the Spergel et al paper, also in 2003, shows the final results from WMAP using this analysis.

It is a tortuous path from theory to observation. I did find a good lecture from the summer school on cosmology from ICTP in 2016 (https://www.youtube.com/watch?v=wdOUiPicWM8) which did link all these approaches together. So, I think I am more or less there in understanding this area at the level I am happy with.
 
  • #15
kimbyd said:
It is difficult to track through the whole thought process for why the CMB is such powerful evidence for dark matter, but it is all there. Max Tegmark's movies linked above provide a nice visual for how dark matter influences the CMB (basically, it changes the even/odd peak structure). And the Seljak and Zaldarriaga paper demonstrates how that link is calculated in practice (if you want to trace the calculations back, they also provide references for how dark matter was originally included).

Finally, if you're concerned about how dark matter is "assumed" from the start, bear in mind that if dark matter didn't exist, the above analysis procedure would measure its density to be zero. It doesn't.

I have spotted an interesting conundrum with the Mark Tegmark movie in that let one label the peaks 1 to 7; at low baryon fraction you have only peaks 1-3 with 4 and 5 beginning to appear. As the baryon fraction increases, peak 1 increases but peak 2 decreases and eventually almost disappears. The lower peaks 4-7 become progressively more apparent as the baryon fraction increases. So the question is: which peak is the second peak in the WMAP data is it peak 2 or 3 with a now absent peak 2, indicating a greatly increased baryon fraction that the current standard model assumes.
 
  • #16
Adrian59 said:
I have spotted an interesting conundrum with the Mark Tegmark movie in that let one label the peaks 1 to 7; at low baryon fraction you have only peaks 1-3 with 4 and 5 beginning to appear. As the baryon fraction increases, peak 1 increases but peak 2 decreases and eventually almost disappears. The lower peaks 4-7 become progressively more apparent as the baryon fraction increases. So the question is: which peak is the second peak in the WMAP data is it peak 2 or 3 with a now absent peak 2, indicating a greatly increased baryon fraction that the current standard model assumes.
There are two important effects that are necessary to understand what this is doing to the power spectrum:
1) The acoustic oscillations themselves which set up the interference pattern. For pure baryonic matter, the odd and even peaks will be of equivalent primordial magnitude. If there is much dark matter, the even-numbered peaks are suppressed.
2) The surface of last scattering, which is marked by the transition of the early universe from a plasma to a gas state, did not happen instantaneously. It took a few hundred thousand years. This has the impact of blurring the CMB signal, suppressing power at small angular scales.

The combination of these two effects means that you need to measure, at a minimum, the first three peaks of the CMB to get a positive determination of the ratio of normal matter to dark matter. The first two peaks alone don't get you very far, because the second peak will always be measured to be smaller than the first. The third peak, however, if there is nothing but baryonic matter, will be smaller still than the second peak. This isn't the case in our universe: the third peak is roughly the same magnitude as the second, despite the blurring introduced by the fact that the plasma to gas phase transition wasn't instantaneous.
 
  • #17
kimbyd said:
There are two important effects that are necessary to understand what this is doing to the power spectrum:
1) The acoustic oscillations themselves which set up the interference pattern. For pure baryonic matter, the odd and even peaks will be of equivalent primordial magnitude. If there is much dark matter, the even-numbered peaks are suppressed.
2) The surface of last scattering, which is marked by the transition of the early universe from a plasma to a gas state, did not happen instantaneously. It took a few hundred thousand years. This has the impact of blurring the CMB signal, suppressing power at small angular scales.

The combination of these two effects means that you need to measure, at a minimum, the first three peaks of the CMB to get a positive determination of the ratio of normal matter to dark matter. The first two peaks alone don't get you very far, because the second peak will always be measured to be smaller than the first. The third peak, however, if there is nothing but baryonic matter, will be smaller still than the second peak. This isn't the case in our universe: the third peak is roughly the same magnitude as the second, despite the blurring introduced by the fact that the plasma to gas phase transition wasn't instantaneous.

However, in the Mark Tegmark movie it appears that the even peaks decrease with increasing baryons, so assuming a fixed matter component, dark matter will be decreasing not increasing as the even peaks are progressively depressed. Purely by chance I found a paper by Stacy S. McGaugh from 1999, 'Distinguishing Between CDM and MOND: Predictions for the Microwave Background' which does report exactly what I have observed with disappearing even peaks of the CMBR depending on what cosmological model you are using. Interestingly, and here I am stating up front that I am not a supporter of MOND, this paper shows how CMBR anisotropies can be explained in a MONDian universe!
 
  • #18
Adrian59 said:
However, in the Mark Tegmark movie it appears that the even peaks decrease with increasing baryons, so assuming a fixed matter component, dark matter will be decreasing not increasing as the even peaks are progressively depressed. Purely by chance I found a paper by Stacy S. McGaugh from 1999, 'Distinguishing Between CDM and MOND: Predictions for the Microwave Background' which does report exactly what I have observed with disappearing even peaks of the CMBR depending on what cosmological model you are using. Interestingly, and here I am stating up front that I am not a supporter of MOND, this paper shows how CMBR anisotropies can be explained in a MONDian universe!
What movies are you looking at? I'm not entirely sure that I see any of them that are really good at showing this result. The combo movies don't show small enough angular scales to really show what's going on (only the first two peaks are visible for most of the "Baryons" movie). The old movies may be misleading due to them not showing what the other parameter choices were.
 
  • #19
BTW, NASA has a site where you can put in your own parameter choices and get out an estimate of the CMB power spectrum. It's quite complicated (lots and lots of parameters go into these models), but fairly quick to use:
https://lambda.gsfc.nasa.gov/toolbox/tb_camb_form.cfm

I did a simple run where I set the Baryon density to the current measured sum of the dark matter and baryon densities, and set the dark matter density to zero. The link to the results is here, though I don't know if it's accessible by others:
https://lambda.gsfc.nasa.gov/tmp/camb/camb_27375040.cfm

In case the above link doesn't work, I've attached the plot:
cmb_no_dm.png


As you can clearly see, the peaks decrease monotonically in amplitude, with no even/odd variation visible at all.
 

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  • #20
kimbyd said:
What movies are you looking at? I'm not entirely sure that I see any of them that are really good at showing this result. The combo movies don't show small enough angular scales to really show what's going on (only the first two peaks are visible for most of the "Baryons" movie). The old movies may be misleading due to them not showing what the other parameter choices were.

I was looking at your reference http://space.mit.edu/home/tegmark/cmb/movies.html though this observation was in the section marked CMB movies old. Also, the graphic changes quite rapidly so to see what is happening your have to freeze the frame at different points.
 
  • #21
Adrian59 said:
I was looking at your reference http://space.mit.edu/home/tegmark/cmb/movies.html though this observation was in the section marked CMB movies old. Also, the graphic changes quite rapidly so to see what is happening your have to freeze the frame at different points.
Yeah, I'm quite sure the "Baryons" movie there uses a model which has a lot of dark matter.

The "Baryons" movie in the "Combo Movies" section is far more representative (since it keeps ##\omega_b + \omega_d## constant), but you can't see the effect I described because the scale of the graph is off.
 

Related to CMBR anisotropy and cosmic abundances

1. What is CMBR anisotropy?

CMBR anisotropy refers to the small variations in temperature observed in the cosmic microwave background radiation (CMBR) across the sky. These variations provide important clues about the structure and evolution of the universe.

2. How is CMBR anisotropy measured?

CMBR anisotropy is measured using specialized instruments, such as telescopes and satellites, that are designed to detect and map the tiny temperature fluctuations in the CMBR. These measurements are then analyzed to determine the pattern and magnitude of the anisotropy.

3. What causes CMBR anisotropy?

The primary cause of CMBR anisotropy is the expansion of the universe and the resulting changes in the density of matter and radiation. Other factors, such as the presence of dark matter and the effects of gravitational lensing, can also contribute to the observed anisotropy.

4. What can we learn from CMBR anisotropy?

CMBR anisotropy provides valuable insights into the early universe and the processes that shaped its evolution. By studying the patterns of anisotropy, scientists can better understand the distribution and properties of matter and energy, as well as the overall structure and geometry of the universe.

5. How does CMBR anisotropy relate to cosmic abundances?

The distribution of matter and energy in the universe, as revealed by CMBR anisotropy, is closely linked to the relative abundances of different elements and particles. By studying the anisotropy, scientists can gain a better understanding of how these abundances have changed over time and how they are affected by various physical processes.

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