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It is said that CMBR indicates that dark matter is non-baryonic. How so?
A lot on the net about this if you Google, 'Dark matter non baryonic.'Ranku said:It is said that CMBR indicates that dark matter is non-baryonic. How so?
Try googling baryon loading CMB. The following seems to be a decent non-mathematical exposition:Ranku said:It is said that CMBR indicates that dark matter is non-baryonic. How so?
It would be more accurate to say that the CMBR is consistent with a universe with non-baryonic dark matter, than that it "indicates" that this is the case.Ranku said:It is said that CMBR indicates that dark matter is non-baryonic. How so?
I haven't seen any modified gravity theory which comes close to reproducing the CMBR power spectrum without dark matter. It seems quite unlikely to me to be possible given the nature of the physics involved.ohwilleke said:It would be more accurate to say that the CMBR is consistent with a universe with non-baryonic dark matter, than that it "indicates" that this is the case.
This is because the CMBR peaks seen could also have another BSM source than non-baryonic dark matter (e.g. some modified gravity theories).
You would be wrong in thinking that, although its a quite reasonable thing to assume. See, e.g.:kimbyd said:I haven't seen any modified gravity theory which comes close to reproducing the CMBR power spectrum without dark matter. It seems quite unlikely to me to be possible given the nature of the physics involved.
I haven't read the papers for a while and never with those specific details in mind. All of them are linked with open access full text papers available. Feel free to review them yourself. You can eyeball the charts above as well.Hyperfine said:Did any of the papers listed immediately above provide a fit to the TE cross-correlation power spectrum? I am curious about their fits to the dip in that power spectrum in the region of multipole moments of 100.
And yet to summarily dismiss a question regarding fits to an observed CMB power spectrum.ohwilleke said:Indeed, it is reasonable to hypothesize, based upon these examples, that almost any modified gravity theory that can reproduce flat rotation curves will, in its relativistic generalization, reproduce the CMB peaks.
In that case of ACG 114905, the most likely cause is an angle of inclination measurement error in the initial assessment that it is Keplerian (an uncertainty that the initial paper describing ACG 114905 as a Keplerian galaxy itself identifies as a potential source of a serious problem with its assessment), citing Banik et. al. (2022) titled, “Overestimated inclinations of Milgromian disc galaxies: the case of galaxy AGC 114905“.Hyperfine said:And yet to summarily dismiss a question regarding fits to an observed CMB power spectrum.
In addition, how do these proposed theories treat observed galactic rotation curves that are Keplerian? For example AGC 114905? Reference: https://arxiv.org/abs/2112.00017
Actually, the 3rd peak was predicted by McGaugh in 1990 or so in MOND before ΛCDM.kimbyd said:I haven't seen any modified gravity theory which comes close to reproducing the CMBR power spectrum
Given how soon BBN occurs after the Big Bang (up to about ca. 15 minutes), it could be that the background gravitational field almost everywhere is greater than the MOND constant a0, in which case, it would have no effect.Vanadium 50 said:Where I think this might get interesting is coupling this with BBN. Both models will likely reproduce the observed 4He fraction, as that is hard to move, what do they do with deuterium and lithium?
This one uses a TeVeS theory where the scalar component is contrived to mimic dark matter (that is, its energy density scales close to ##1/a^3##). I guess I'm not terribly surprised this could replicate the CMB data, as it's basically an alternative form of dark matter theory.ohwilleke said:You would be wrong in thinking that, although its a quite reasonable thing to assume. See, e.g.:
Constantinos Skordis, Tom Złosnik, "A new relativistic theory for Modified Newtonian Dynamics" arXiv (June 30, 2020) (127 Phys. Rev. Lett. 161302 (2021)).
This one isn't a modified gravity theory at all. It's a claim that actually, physicists have been doing General Relativity calculations incorrectly, and doing them the right way, according to this author, removes the need for both dark matter and dark energy. Suffice it to say I am very skeptical.ohwilleke said:A. Deur, "Effect of the field self-interaction of General Relativity on the Cosmic Microwave Background Anisotropies"
arXiv:2203.02350 (March 4, 2022) (39 Class. Quantum Grav. 135003 (2022)).
Your link is broken for this one. Here is a link that I found:ohwilleke said:W.M. Stuckey, Timothy McDevitt, A.K. Sten, Michael Silberstein, "The Missing Mass Problem as a Manifestation of GR Contextuality" 27(14) International Journal of Modern Physics D 1847018 (2018). DOI: 10.1142/S0218271818470181.
Perhaps in terms of the overall structure, but I don't believe it is able to reproduce the CMB in detail. Similar to the above theory which sorta works, but gets the parameters way off.Vanadium 50 said:Actually, the 3rd peak was predicted by McGaugh in 1990 or so in MOND before ΛCDM.
It isn't a TeVeS theory (that theory was by the late professor Bekenstein who was a colleague of Milgrom; the theory's name is a Hebrew pun). But, it is a different relativistic generalization of MOND. It is not an alternative form of dark matter theory.kimbyd said:This one uses a TeVeS theory where the scalar component is contrived to mimic dark matter (that is, its energy density scales close to ##1/a^3##). I guess I'm not terribly surprised this could replicate the CMB data, as it's basically an alternative form of dark matter theory.
Whether it is truly incorporating an overlooked GR effect (specifically, the self-interaction of the gravitational field), or it is actually a modification of gravity, it doesn't matter much, because the fact is that it works exquisitely well to reproduce the observations.kimbyd said:This one isn't a modified gravity theory at all. It's a claim that actually, physicists have been doing General Relativity calculations incorrectly, and doing them the right way, according to this author, removes the need for both dark matter and dark energy. Suffice it to say I am very skeptical.
I don't have the expertise to be able to identify any problems with the theory, but it doesn't look like this person's papers have been interacted with much at all by the broader cosmology/GR community either, so it's hard to say what other theorists think of these pretty outlandish claims.
Apologies for the bad link. Probably fat fingers on my part. Thanks for finding a good link.kimbyd said:Your link is broken for this one. Here is a link that I found:
https://arxiv.org/abs/1509.09288
I really don't like the theoretical approach they're taking. They're basically saying that they're not modifying gravity, and then proceed to modify gravity. It's just weird.
But the bigger problem is that their fit parameters to get that CMB graph don't match the cosmology from the nearby universe (basically they have a far, far larger Hubble tension than we currently see with ΛCDM).
Deur's approach isn't a GR modification. We show here that within GR’s formalism, these terms can be regrouped in an overall term D(z) factoring the right hand side of Eq. (9). Instead Deur drops the cosmological principle, see his modified Friedmann equations (9) and (14), representing an inhomogeneous and anisotropic universe.ohwilleke said:So, if Deur's approach turns out that it is actually a GR modification, rather than correctly being described as an overlooked GR effect, who cares?
One thing that's missing from this, though, is an actual derivation of those modified equations from the field equation. I don't see that anywhere; Deur just asserts equations (10), (11), (12), and (13) without argument or derivation.timmdeeg said:Deur's approach isn't a GR modification. We show here that within GR’s formalism, these terms can be regrouped in an overall term D(z) factoring the right hand side of Eq. (9).
Isn't there literature describing how equation (5) based on assuming the cosmological principle evolves to a modified equation if that principle is dropped? To me equation (10) seemed a bit like hand-waving. I wonder if the property "anisotropy" can be described by a single number with a correction factor as shown in equation (10), but thought that's still text book physics.PeterDonis said:One thing that's missing from this, though, is an actual derivation of those modified equations from the field equation. I don't see that anywhere; Deur just asserts equations (10), (11), (12), and (13) without argument or derivation.
I believe there are papers treating models that are not isotropic or homogeneous, but I don't have any specific references.timmdeeg said:Isn't there literature describing how equation (5) based on assuming the cosmological principle evolves to a modified equation if that principle is dropped?
Possibly, if Deur says "... , these terms can be regrouped in an overall term D(z) factoring the right hand side of Eq. (9)." doesn't mean more that D(z) stands for a deviation from homogeneity and isotropy without referencing to a specific model. As such it is not a derivation.PeterDonis said:One thing that's missing from this, though, is an actual derivation of those modified equations from the field equation. I don't see that anywhere; Deur just asserts equations (10), (11), (12), and (13) without argument or derivation.
Ranku said:It is said that CMBR indicates that dark matter is non-baryonic. How so?
kimbyd said:The basic reason is because before the CMB was emitted, the universe was a plasma. While the universe was a plasma, baryonic matter experienced pressure. This meant that on large scales, when normal matter fell into a gravitational potential well, the pressure would cause it to bounce back. Dark matter, on the other hand, doesn't experience pressure and so can't bounce.
This leads to a very clear signal in the power spectrum of the CMB, where the even-numbered peaks are suppressed because of the lack of bouncing (dark matter contributes to only the odd-numbered peaks on the CMB).
Dark Mather is a real headache to understandkimbyd said:The basic reason is because before the CMB was emitted, the universe was a plasma. While the universe was a plasma, baryonic matter experienced pressure. This meant that on large scales, when normal matter fell into a gravitational potential well, the pressure would cause it to bounce back. Dark matter, on the other hand, doesn't experience pressure and so can't bounce.
This leads to a very clear signal in the power spectrum of the CMB, where the even-numbered peaks are suppressed because of the lack of bouncing (dark matter contributes to only the odd-numbered peaks on the CMB).
A number of years ago, Max Tegmark put together a series of videos which show how various parameters impact the CMB power spectrum, if you want a more detailed picture of this:
https://space.mit.edu/home/tegmark/cmb/movies.html
CMBR stands for cosmic microwave background radiation, which is the leftover radiation from the Big Bang. This radiation is uniform in all directions and provides a snapshot of the early universe. Scientists have used observations of the CMBR to study the distribution of matter in the universe. The patterns of the CMBR suggest that there is more matter in the universe than can be explained by visible matter, leading to the concept of dark matter. Non-baryonic dark matter refers to matter that does not consist of protons and neutrons, the building blocks of visible matter. The presence of dark matter is inferred from the gravitational effects it has on visible matter, and the CMBR provides evidence for its existence through its effect on the distribution of matter in the universe.
Dark matter and visible matter have very different properties. Visible matter is made up of particles called baryons, such as protons and neutrons. These particles interact with light and other forms of electromagnetic radiation, making them detectable through telescopes. Dark matter, on the other hand, does not interact with light and is therefore invisible. It is believed to be made up of particles that do not interact with electromagnetic radiation, making it difficult to detect and study.
Scientists have proposed several candidates for non-baryonic dark matter, including weakly interacting massive particles (WIMPs), sterile neutrinos, and axions. WIMPs are particles that interact with gravity and other fundamental forces, but very weakly with visible matter. Sterile neutrinos are hypothetical particles that do not interact with any of the known fundamental forces except gravity. Axions are another proposed candidate, and they are particles that were originally proposed to explain why the strong nuclear force is symmetrical in both directions of time.
The CMBR is an important tool for studying the distribution of matter in the universe. Scientists use observations of the CMBR to create maps of the temperature fluctuations in the early universe. These maps show that there are areas of higher and lower density in the universe. By comparing these maps to models of the universe, scientists can determine the amount and distribution of dark matter. The presence of dark matter is inferred from the gravitational effects it has on visible matter, which can be seen in the patterns of the CMBR.
The discovery of non-baryonic dark matter through CMBR evidence has significant implications for our understanding of the universe. It suggests that there is more to the universe than what we can see, and that there are fundamental particles and forces that we have yet to discover. It also has implications for our understanding of the formation and evolution of galaxies, as dark matter plays a crucial role in the structure and dynamics of these systems. Furthermore, the search for dark matter can provide insights into the nature of the universe and potentially lead to new discoveries in physics.