Some questions regarding WIMPs as a DM candidate

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The discussion centers on the detection of Weakly Interacting Massive Particles (WIMPs) as dark matter candidates. Key points include the confusion surrounding the distribution of WIMPs, which are believed to cluster in galactic halos but also exhibit high density in galaxy clusters due to their gravitational interactions. The concept of WIMPs moving like a "wind" is clarified, noting that while they don't rotate significantly around the galactic center, their relative motion to the sun creates a detectable flux. Additionally, the potential for indirect detection through high-energy gamma-rays is discussed, with questions raised about the mass boundaries of WIMPs. Overall, the conversation highlights the complexities of dark matter distribution and detection methods.
  • #31
SpaceTiger said:
Do you have an academic reference for this? Last I checked, it couldn't fit the CMB.
I only have this week's New Scientist article to go on. They quote Constantinos Skordis of the Perimeter Institute in Waterloo Ontario Physical Review Letters vol 96 011301, but I have not seen that paper.

The article also has a WMAP power spectrum diagram with the mainstream and MOND predicted curves, which you may want to examine (NS 29 April 06 page 54).

Garth
 
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  • #32
I have now found that Skordis et al. paper on the arXiv: Large Scale Structure in Bekenstein's theory of relativistic Modified Newtonian Dynamics
Since the baryon content is set by the abundance of light elements, we must compensate with a high value of the cosmological constant, i.e. with \Omega_{\Lambda} \sim 0.95. An obvious consequence of this is that the angular-distance relation will be modified as compared to the standard adiabatic \LambdaCDM universe [11]. Indeed the position of the peaks in the angular power spectrum of the CMB will be shifted to higher ls which would lead to a severe mismatch with the current available data from the Wilkinson Microwave Anisotropy Probe and other experiments. A natural solution to this is to include a small component of massive neutrinos, \Omega_{\nu} \sim 0.15. As we can see in the top panel of Fig. 4, with this modification we can reproduce the temperature anisotropy data.

So they get rid of DM in galaxies and clusters by introducing an enormous DE component and a substantial cosmological density component of massive neutrinos...

There you go, another DM candidate! - But I thought the neutrino mass has been established to only allow \Omega_{\nu} \sim 0.01?

Garth
 
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  • #33
Garth said:
Actually the TeVeS version of MOND is undergoing a revival see an article in the latest New Scientist Gravity: Were Newton and Einstein wrong?
It's a long-standing question whether his law of gravity, supposed to explain everything from falling apples to spinning galaxies, might actually be flawed. That is the claim of a growing number of physicists who support a controversial alternative theory called modified Newtonian dynamics or MOND..."From being really out in the cold from a theoretical point of view, MOND is now being taken very seriously," said University of Oxford physicist James Binney
Just some further information from James Binney's homepage
James Binney graduated with a BA from Cambridge University in 1971, and with a doctorate from Oxford University in 1975. From 1975{1979 he was a Fellow by Examination of Magdalen College, Oxford. During 1976 he was a Lindemann Fellow at Princeton University, whither he returned in 1979 as a Visiting Assistant Professor in Astrophysical Sciences. In 1981 he became University Lecturer, and in March 1990 Ad Hominem Reader in Theoretical Physics at Oxford University. In July 1996 he became Professor of Physics at Oxford University. From 1981 he has been a Fellow and Tutor in Physics of Merton College, Oxford.

Garth
 
  • #34
But I thought the neutrino mass has been established to only allow \Omega_{\nu}<0.01

I think that limit is assuming \Lambda CDM.

Their fit to the power spectrum looks very strange. They seem to be fitting to a combination of first- and third-year WMAP data (strange, since the third-year includes the first-year) and ignoring results from other experiments. Even with neutrinos, their model produces a small third peak that would probably be inconsistent with other CMB experiments.
 
  • #35
I concur; a wicked thought: perhaps they need to add another field, say a spinor field? With enough fields and tunable parameters I am sure they will eventually be able to make it fit. The ad hoc nature of the theory and the specific required values of those parameters could always be explained as an anthropic coincidence!

Of course this might be seen as 'epicycle fitting'... :wink:

Garth
 
  • #36
Whenever someone brings up MOND, I always like to post a link to this paper;
"Direct constraints on the dark matter self-interaction cross-section from the merging galaxy cluster 1E0657-56"
http://arxiv.org/abs/astro-ph/0309303"

The basic gist is the comparison of a Chandra x-ray image and a lensing map of the "bullet cluster". The MOND people agree that the majority of baryonic matter in a cluster is in the intra-cluster medium , so this begs the question; Why do we see a lensing map consisitent with the majority of the mass being offset from the gas in the merging subcluster? Interestingly, mass contours overlay an optically detected galaxy overdensity, presumably the infalling cluster galaxies, which lies in front of the gas which has been ram-pressure stripped from the galaxies by its interaction with the main cluster gas (the galaxies are collisionless). Fair evidence against MOND?
 
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  • #37
matt.o said:
Whenever someone brings up MOND, I always like to post a link to this paper;
"Direct constraints on the dark matter self-interaction cross-section from the merging galaxy cluster 1E0657-56"
http://arxiv.org/abs/astro-ph/0309303"

The basic gist is the comparison of a Chandra x6ray image and a lensing map of the "bullet cluster". The MOND people agree that the majority of baryonic matter in a cluster is in the intra-cluster medium , so this begs the question; Why do we see a lensing map consisitent with the majority of the mass being offset from the gas in the merging subcluster? Interestingly, mass contours overlay an optically detected galaxy overdensity, presumably the infalling cluster galaxies, which lies in front of the gas which has been ram-pressure stripped from the galaxies by its interaction with the main cluster gas (the galaxies are collisionless). Fair evidence against MOND?

What about Lagrange points at the Galactic scale (I'm not sure if they exist - there's objects from many angles)? What happens to weak lensing at Lagrange points where orbits are strong (probably nothing right)? Could the Lagrange points have an affect on how the gas and matter behave?
 
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  • #38
matt.o said:
Whenever someone brings up MOND, I always like to post a link to this paper;
"Direct constraints on the dark matter self-interaction cross-section from the merging galaxy cluster 1E0657-56"
http://arxiv.org/abs/astro-ph/0309303"

The basic gist is the comparison of a Chandra x-ray image and a lensing map of the "bullet cluster". The MOND people agree that the majority of baryonic matter in a cluster is in the intra-cluster medium , so this begs the question; Why do we see a lensing map consisitent with the majority of the mass being offset from the gas in the merging subcluster? Interestingly, mass contours overlay an optically detected galaxy overdensity, presumably the infalling cluster galaxies, which lies in front of the gas which has been ram-pressure stripped from the galaxies by its interaction with the main cluster gas (the galaxies are collisionless). Fair evidence against MOND?
Yes, thank you matt-o for that link. From that paper:
2.1. The gas — dark matter offset
The most remarkable feature in Fig. 1b is a ∼ 23′′ offset between the subcluster’s DM centroid and the gas bullet, which is at least 2\sigma-significant (C04). C04 use this fact as a direct proof of dark matter existence, as opposed to modified gravity hypotheses (Milgrom 1983 and later works) in which one would expect the lensing mass peak to be associated with the gas — the dominant visible mass component.
but note it concludes:
Finally, we note that our limit, \sigma/m < 1 cm2 g-1, excludes most of the 0.5 - 5 cm2 g-1 interval proposed to explain the flat mass profiles in galaxies. Within the SIDM paradigm, the galaxy profiles and the tight cross-section limits coming from clusters can still be reconciled if the cross-section were velocity-dependent, so that it would be smaller on average in clusters than in galaxies (e.g., Firmani et al. 2000, 2001;Hennawi & Ostriker 2002; Colín et al. 2002). However, it is difficult to justify this additional degree of freedom in the model until a nonzero cross-section is detected at any velocity.
(emphasis mine)

How does this square with weakly interacting DM required to fit non-cuspy halo centres?

Garth
 
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  • #39
SpaceTiger said:
But I thought the neutrino mass has been established to only allow \Omega_\nu < 0.01
I think that limit is assuming \Lambda CDM.
Isn't that just assuming h ~ 0.73, i.e. \Omega_\nu h^2 \sim 0.02, rather than the rest of the model?

Garth
 
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  • #40
Garth said:
Isn't that just assuming h ~ 0.73, i.e. \Omega_\nu h^2 \sim 0.02, rather than the rest of the model?

I believe the limit is obtained by constraining the effect of neutrinos on the CMB power spectrum (as well as the growth of large-scale structure). They couldn't make this constraint without simultaneously fitting other parameters and I assume they would have used the usual ones (with \Lambda, CDM, etc.).
How does this square with weakly interacting DM required to fit non-cuspy halo centres?

It's still not entirely clear whether or not the "cusp" problem is actually a problem. If it is, self-interacting dark matter is one possible solution, but it's not the only one.
 
  • #41
SpaceTiger said:
I believe the limit is obtained by constraining the effect of neutrinos on the CMB power spectrum (as well as the growth of large-scale structure). They couldn't make this constraint without simultaneously fitting other parameters and I assume they would have used the usual ones (with \Lambda, CDM, etc.).
Yes, the \LambdaCDM limit for an individual neutrino mass is about 0.3 eV, but I was thinking of direct laboratory measurement such as by the Super-Kamiokande neutrino detector & the http://ej.iop.org/links/q81/ftMTkHWSKK1+w6fGYyfRdg/jhep022003009.pdf & MINOS experiments which were consistent with the heaviest neutrino being at least 0.05 electron volts, but no more than 0.3 electron volts.

Garth
 
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  • #42
Yes, the LCDM limit for an individual neutrino mass is about 0.3 eV

LCDM gives a limit on the sum of the neutrino masses (all flavors).


Garth said:
experiments which were consistent with the heaviest neutrino being at least 0.05 electron volts, but no more than 0.3 electron volts.

Where in the papers do they say that? I was under the impression that these experiments measured the difference in neutrino masses. I know there are upper limits on the neutrino mass at around 0.3 electron volts from other experiments, but I'm not aware of any lower limits.
 
  • #43
SpaceTiger said:
LCDM gives a limit on the sum of the neutrino masses (all flavors).
Garth said:
experiments which were consistent with the heaviest neutrino being at least 0.05 electron volts, but no more than 0.3 electron volts.
Where in the papers do they say that? I was under the impression that these experiments measured the difference in neutrino masses. I know there are upper limits on the neutrino mass at around 0.3 electron volts from other experiments, but I'm not aware of any lower limits.
From Neutrino Masses and Mixing: Evidence and Implications
The evidence for neutrino masses implies that the SM cannot be a complete picture of Nature. In particular, if the SM is only a low energy effective theory, very light neutrino masses are expected. The scale at which the SM picture is not valid anymore is inversely proportional to the scale of neutrino masses. Specifically
mν >~ sqrt {\triangle m2atm} ∼ 0.05 eV
(Page 87)

Garth
 
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  • #44
It looks like that's a mass scale for the breakdown of the standard model, not an experimental limit on the neutrino mass.
 
  • #45
I think you are dead wrong on this count, Garth. MOND is just plain wrong IMO. Any attempt to apply MOND to WMAP3 gives horrid results. I have attempted to give MOND the benefit of the doubt, but not anymore. It looks like grasping at straws to me.
 
  • #46
Chronos said:
I think you are dead wrong on this count, Garth. MOND is just plain wrong IMO. Any attempt to apply MOND to WMAP3 gives horrid results. I have attempted to give MOND the benefit of the doubt, but not anymore. It looks like grasping at straws to me.
You are mis-reading me, having reported the NS article I disagree with it and agree with you Chronos - as I posted above from matt-o's paper "Direct constraints on the dark matter self-interaction cross-section from the merging galaxy cluster 1E0657-56" http://arxiv.org/abs/astro-ph/0309303
C04 use this fact as a direct proof of dark matter existence, as opposed to modified gravity hypotheses

however they then say
excludes most of the 0.5 - 5 cm2 g-1 interval proposed to explain the flat mass profiles in galaxies
which then might leave a problem for the standard model of DM as well.

Garth
 
  • #47
Garth said:
however they then say which then might leave a problem for the standard model of DM as well.

Interacting dark matter is not part of the standard model, by any means. The standard for CDM simulations is always non-interacting dark matter.
 
  • #48
SpaceTiger said:
It looks like that's a mass scale for the breakdown of the standard model, not an experimental limit on the neutrino mass.
Well, they measure the difference in mass between the different types of neutrinos in various oscillation experiments and use theory to predict their absolute masses, so that lower mass detection is theory dependent on the standard particle model as is the upper mass determination from the WMAP data dependent on the standard cosmological model.

Garth
 
  • #49
Well, they measure the difference in mass between the different types of neutrinos in various oscillation experiments and use theory to predict their absolute masses

Actually, I think they're just assuming that none of the neutrinos can have a mass < 0 and taking the measured mass difference to be the lower limit on the neutrino mass. It's the inferred difference in mass that depends on the standard model mixing-matrix formalism.

Anyway, I agree that the lower limit would have to be in that ballpark. I had forgotten that atmospheric neutrinos were giving such a large mass difference.
 
  • #50
SpaceTiger said:
Interacting dark matter is not part of the standard model, by any means. The standard for CDM simulations is always non-interacting dark matter.
Not even to solve the 'cuspy halo problem? http://www.journals.uchicago.edu/ApJ/journal/issues/ApJ/v547n2/52142/52142.text.html ?
We find, in agreement with various authors, that CDM (collisionless cold dark matter) yields cuspy halos that are too centrally concentrated as compared to observations
(Italics mine)

Garth
 
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  • #51
Garth said:
Not even to solve the 'cuspy halo problem?

As I said before, there's no standard solution to that problem and the fact that it's getting less severe with time suggests that it may have just been an artifact of imperfect cosmological simulations. We shouldn't ignore it, but that doesn't mean that evidence against self-interacting dark matter is evidence against the standard model, by any stretch of the imagination.
 
  • #52
Are we back to the OP? Do these constraints rule out WIMPs?

If so what alternatives are left that solve the mass cluster distribution and flat galactic centre distribution?

Garth
 
  • #53
Garth said:
Are we back to the OP? Do these constraints rule out WIMPs?

If so what alternatives are left that solve the mass cluster distribution and flat galactic centre distribution?

Why would they rule out WIMPs?
 
  • #54
SpaceTiger said:
Why would they rule out WIMPs?
Your statement:
The standard for CDM simulations is always non-interacting dark matter.

Perhaps I am confused. Does you use of the term 'non-interacting' particles include 'weakly interacting' WIMPS?

Garth
 
  • #55
Garth said:
Perhaps I am confused. Does you use of the term 'non-interacting' particles include 'weakly interacting' WIMPS?

"Non-interacting" basically means "interacting so weakly (with both itself and its environment) that the effects are not noticable". Self-interacting dark matter, on the other hand, hypothesizes relatively strong interactions between dark matter particles, but weak interactions with everything else.
 
  • #56
SpaceTiger said:
"Non-interacting" basically means "interacting so weakly (with both itself and its environment) that the effects are not noticable". Self-interacting dark matter, on the other hand, hypothesizes relatively strong interactions between dark matter particles, but weak interactions with everything else.
Thank you for that clarification, so WIMPS are non-interacting then.

Garth
 
  • #57
Garth said:
Thank you for that clarification, so WIMPS are non-interacting then.

For cosmological purposes, yes. They still have non-zero cross sections, they're just small enough as to be dynamically negligible.
 
  • #58
Its a pleasure watching Garth talk with ST, this is such a vibrant conversation between two brilliant people. I love this.
 

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