Solving Dark Matter with SUSY Theory

In summary: If you plug in numbers for a DM particle of mass 10...The time it would take for the DM particle to decay into a singleton would be 10^(-18) years.
  • #1
varphi42
5
0
Hello,

How could SUSY provides a candidate to dark matter since it would only appear only above the TeV scale? The galaxies' environments is at such energies?

Thanks
 
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  • #2
I think this is an answer to this question : the lightest supersymmetric particle (LSP) could be a massive and stable one with no color and no charge.
 
  • #3
varphi42 said:
I think this is an answer to this question : the lightest supersymmetric particle (LSP) could be a massive and stable one with no color and no charge.

The idea is that the dark matter particles were generated during the big bang when the average energy of the particles making up the universe (i.e. temperature) was larger than the mass of the LSP. As the temperature of the universe dropped below that point, these particles "froze out" and, since they are stable, they have just been carried along ever since, only interacting gravitationally.
 
  • #4
phyzguy said:
The idea is that the dark matter particles were generated during the big bang when the average energy of the particles making up the universe (i.e. temperature) was larger than the mass of the LSP. As the temperature of the universe dropped below that point, these particles "froze out" and, since they are stable, they have just been carried along ever since, only interacting gravitationally.

If that's true, and production of dark matter ceased soon after the Big Bang, than the average density of dark matter should be decreasing with the expansion of the universe. And this should be measurable in terms of microlensing. Right?
 
  • #5
friend said:
If that's true, and production of dark matter ceased soon after the Big Bang, than the average density of dark matter should be decreasing with the expansion of the universe.

Yes, this is absolutely the case. Note that the average density of ordinary matter is also decreasing at the same rate as the universe expands.

friend said:
And this should be measurable in terms of microlensing. Right?

Not necessarily. The density of gravitationally bound objects, like stars and galaxies, does not decrease as the universe expands. Microlensing refers to lensing by compact objects like stars and planets, and their density is not changing.
 
  • #6
phyzguy said:
Yes, this is absolutely the case. Note that the average density of ordinary matter is also decreasing at the same rate as the universe expands.

Not necessarily. The density of gravitationally bound objects, like stars and galaxies, does not decrease as the universe expands. Microlensing refers to lensing by compact objects like stars and planets, and their density is not changing.

As I understand it, dark matter does not clump. But I see nothing to prevent it from orbiting around each other in tighter and tighter orbits as it looses energy due to gravitational radiation. And maybe there is a history of this in the microlensing.
 
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  • #7
Dark matter most certainly does clump. What it does not do is clump on scales small compared to a galaxy. While galactic formation is not entirely understood, it is commonly believed that galaxies form in regions of high dark matter density. In any event, this idea of dark matter "orbiting around each other in tighter and tighter orbits as it looses energy due to gravitational radiation" won't work out - if this were to happen outside the galaxy, it would also happen inside the galaxy, and we'd be seeing DM annihilation radiation from the galactic core.
 
  • #8
Vanadium 50 said:
Dark matter most certainly does clump. What it does not do is clump on scales small compared to a galaxy. While galactic formation is not entirely understood, it is commonly believed that galaxies form in regions of high dark matter density. In any event, this idea of dark matter "orbiting around each other in tighter and tighter orbits as it looses energy due to gravitational radiation" won't work out - if this were to happen outside the galaxy, it would also happen inside the galaxy, and we'd be seeing DM annihilation radiation from the galactic core.

I'm trying to consider tests that distinguish whether dark matter is a particle or a gravitational modification. My thoughts are: if it is a particle, then it orbits (by definition), and if it orbits, then it radiates gravitational waves and falls closer to the center of mass. I don't see how that can be avoided for any particle with mass. I think this means that it would eventually gravitate to the center of galaxies. I don't know what that means for its overall distribution.
 
  • #9
You're right that any orbiting particle will lose energy due to gravitational radiation and spiral in. However, the timescale for this to happen is extraordinarily long in the case of dark matter orbiting in galaxies. The timescale for orbital decay is give by:
[tex] \tau = \frac{5c^5 r^4}{256G^3 m_1 m_2(m_1+m_2)}[/tex]

If you plug in numbers for a DM particle of mass 10 GeV, a galaxy of mass 1E12 Msun, and a radius of 1 kpc, this gives an orbital decay timescale of ~10^83 years, a ridiculously long time. Gravitational radiation is negligible except in the case of very massive bodies in very small orbits.
 
  • #10
phyzguy said:
You're right that any orbiting particle will lose energy due to gravitational radiation and spiral in. However, the timescale for this to happen is extraordinarily long in the case of dark matter orbiting in galaxies. The timescale for orbital decay is give by:
[tex] \tau = \frac{5c^5 r^4}{256G^3 m_1 m_2(m_1+m_2)}[/tex]

If you plug in numbers for a DM particle of mass 10 GeV, a galaxy of mass 1E12 Msun, and a radius of 1 kpc, this gives an orbital decay timescale of ~10^83 years, a ridiculously long time. Gravitational radiation is negligible except in the case of very massive bodies in very small orbits.

Thank you. But we don't know how much of the DM orbits on average in the same general location in the same general direction. Some have suggested that there are even small DM dwarf galaxies, that may be orbitting larger visible galaxies. That would change your calculation by quite a bit, I imagine.

Are there other measurable effects of moving matter. Frame dragging comes to mind. If on the average there is a lot of dark matter all orbitting in generally the same direction, then perhaps frame dragging effects may be discernable in the microlensing, right?
 
  • #11
friend said:
Thank you. But we don't know how much of the DM orbits on average in the same general location in the same general direction. Some have suggested that there are even small DM dwarf galaxies, that may be orbitting larger visible galaxies. That would change your calculation by quite a bit, I imagine.

Are there other measurable effects of moving matter. Frame dragging comes to mind. If on the average there is a lot of dark matter all orbitting in generally the same direction, then perhap frame dragging effects my be discernable in the microlensing, right?

The things you mention would change the calculation quite a bit, as you said. But no reasonable assumptions will get it anywhere close to the age of the universe, which is only 10^10 years. You would need to change the calculation by 73 orders of magnitude - this isn't going to happen. Frame dragging is a similarly weak effect which is completely negligible except in the close vicinity of very massive objects.
 
  • #12
phyzguy said:
The things you mention would change the calculation quite a bit, as you said. But no reasonable assumptions will get it anywhere close to the age of the universe, which is only 10^10 years. You would need to change the calculation by 73 orders of magnitude - this isn't going to happen. Frame dragging is a similarly weak effect which is completely negligible except in the close vicinity of very massive objects.

When we are talking potentially about accumulations about 5 times the mass of a host galaxy, I have to think there may be 73 orders of magnitude from a single DM particle. So by comparison with normal matter, should we expect gravitational radiation and/or frame dragging associated with the mass of an entire galaxy? Or is it moving much to slowly for that?
 
  • #13
friend said:
When we are talking potentially about accumulations about 5 times the mass of a host galaxy, I have to think there may be 73 orders of magnitude from a single DM particle. So by comparison with normal matter, should we expect gravitational radiation and/or frame dragging associated with the mass of an entire galaxy? Or is it moving much to slowly for that?

Try putting in the numbers. Give me a proposed m1, m2, and r that brings the gravitational radiation lifetime down to 10^10 years.
 
  • #14
phyzguy said:
Try putting in the numbers. Give me a proposed m1, m2, and r that brings the gravitational radiation lifetime down to 10^10 years.

If you can give me the units of measure used in the formula you gave, I might be able to work with that.

So the question is how close to the supermassive black hole at the center of a galaxy do you have to be in order to notice frame dragging, etc? And could the frame dragging effect be detected by microlensing?
 
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  • #15
friend said:
If you can give me the units of measure used in the formula you gave, I might be able to work with that.

Any units will work as long as you use a consistent set. Try using SI units (effectively the same as MKS units), for a start.
 
  • #16
I don't known so much on DM. Does it gravitate? If yes: does it follow the Newtonian law of motion? If no: can we built a link with some off-shell masses?

Concerning the above discussion: do you mean that a Thiring Lense effect could be the origin for the DM?

Another proposition: do you think DM could be a kind of relativistic effect (similar to the muon time of life problem?) and I mean it does not really exist but is a kind of artefact.

Thanks in advance for answers.
 
  • #17
I'm a little confused about the non-interaction of particles that may have once shared the same symmetry, before some symmetry breaking process occured. I mean when whatever phase transition broke the electroweak symmetry of SU(2)U(1) into the weak-force and the electromagnetic force, the particles of the weak-force still interacted with the particles of the electromagnetic force, right? So if the WIMPs of dark matter once shared a symmetry group with the rest of the standard model particles, why would they not interact now that this symmetry is broken? Does it have to do with the strength of the coupling constant? Then what determines the strength of it?
 

1. What is dark matter and why is it important to solve?

Dark matter is a type of matter that does not interact with light and cannot be directly observed. It makes up about 85% of the total mass in the universe and its presence is necessary to explain the observed gravitational effects on galaxies and galaxy clusters. Solving dark matter is important because it can provide a better understanding of the universe and its evolution.

2. What is SUSY theory and how does it relate to dark matter?

SUSY (Supersymmetry) theory is a theoretical framework that proposes the existence of a new type of particle that is a partner to every known particle in the Standard Model of particle physics. These particles, called supersymmetric particles or sparticles, could be a candidate for dark matter as they do not interact with light and have the potential to explain the observed properties of dark matter.

3. How does SUSY theory explain the observed properties of dark matter?

SUSY theory predicts that the lightest supersymmetric particle (LSP) is stable and interacts weakly with other particles, making it a potential candidate for dark matter. Additionally, the LSP could have the right amount of mass and the right type of interactions to explain the observed gravitational effects of dark matter on galaxies and galaxy clusters.

4. What evidence supports the use of SUSY theory to solve dark matter?

There are several pieces of evidence that support the use of SUSY theory to solve dark matter. One is the observed gravitational effects of dark matter, which can be explained by the existence of a stable and weakly interacting particle like the LSP. Another is the fact that SUSY theory helps to unify and simplify the equations that describe the fundamental forces and particles in the universe.

5. What are the current challenges and limitations of using SUSY theory to solve dark matter?

While SUSY theory is an attractive candidate for solving dark matter, it has not yet been confirmed by experiments. The Large Hadron Collider (LHC) at CERN has not yet found any evidence of supersymmetric particles, which puts constraints on certain models of SUSY theory. Additionally, there are many different SUSY models, making it challenging to determine which one is the correct one to explain dark matter. Further research and experiments are needed to fully understand the role of SUSY theory in solving dark matter.

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