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SUSY and dark matter |
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| May30-12, 12:50 PM | #1 |
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SUSY and dark matter
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 |
| Jul11-12, 09:36 AM | #2 |
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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.
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| Jul11-12, 10:11 AM | #3 |
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| Jul15-12, 04:59 PM | #4 |
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SUSY and dark matter |
| Jul15-12, 07:16 PM | #5 |
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| Jul15-12, 07:54 PM | #6 |
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| Jul15-12, 08:59 PM | #7 |
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Mentor
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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.
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| Jul16-12, 08:42 AM | #8 |
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| Jul16-12, 08:59 AM | #9 |
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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. |
| Jul16-12, 11:58 AM | #10 |
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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? |
| Jul16-12, 12:01 PM | #11 |
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| Jul16-12, 02:47 PM | #12 |
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| Jul16-12, 03:09 PM | #13 |
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| Jul16-12, 04:18 PM | #14 |
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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? |
| Jul16-12, 04:32 PM | #15 |
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| Jul17-12, 04:37 AM | #16 |
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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. |
| Jul17-12, 04:26 PM | #17 |
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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?
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