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Goodbye, dark matter? (updated)

10 o'clock, October 17, 2005

Update: Cosmic Variance has more. Sean, over there, does a good job explaining (for layfolks like myself) exactly what they were trying to say, mathematically, and what was fishy about it. It’s not as simple as the “just use GR” story one gets from skimming the paper.

In a paper that somehow got mentioned in the CERN Courier and on Slashdot, authors Cooperstock and Tieu have suggested that nonlinear effects in GR could explain flat rotation curves in spiral galaxies (one of the historically important pieces of evidence for dark matter). And in two papers, Kolb, Matarrese, Notari and Riotto and then just Kolb, Matarrese, and Riotto have suggested that nonlinear effects in GR could explain the acceleration of the universe (a key piece of evidence for dark energy). Are these people making sense? Are they crazy? Is this worth thinking about? Have they actually explained away the entire dark sector? (Answers: occasionally, possibly, yes, no.)


Our picture of the universe may have just gotten a lot simpler. The major driver behind theories of non-baryonic (that is, not made out of the protons and neutrons that make up you and me and the rest of the observable universe) dark matter was that it seemed impossible to explain the way galaxies rotate without it — the observed motion only made sense if you assumed that the visible galaxy of normal stuff was surrounded by a massive halo of weird stuff.

Now two astrophysicists at the University of Victoria, Fred Cooperstock and Steven Tieu, have published a paper that makes all the weird stuff go away. According to Messrs. C. & T., the Newtonian approximation works well for stuff like the solar system because the planets’ contribution to the overall gravity of the system is so small compared to the sun’s, but it doesn’t work nearly as well for something like a galaxy where all the elements in the system (stars, in this case) contribute more or less equally. For that, they say, you need general relativity — and if you model a galaxy (which they did — ours and three or four others) with general relativity, explaining galactic rotation just with normal matter becomes pretty straightforward.

On the other hand, Mikolaj Korzynski of Warsaw University says that the Cooperstock-Tieu model requires, in addition to stars and dust and whatnot, a giant, infinitely thin disk cutting through the middle of the galaxy like a black hole in the shape of a cookie sheet, and “should therefore be considered unphysical.”

Still, the approach sounds promising. At least, it raises the bar for dark matter — I suspect more than one astrophysicist out there is now feverishly “doing sums” trying to relativistically replicate the Newtonian dark-matter halo model. Good times!

Comments

Egads, David, you're quoting stuff off /astro-ph. Aiiee!

Perhaps due to my teeny amount of self-esteem, I've always been comfortable with the idea that perhaps we see these dark matter halos because our knowledge of gravitation is incomplete. What's more simple and elegant - that we can't see 90% of the universe or that we might just not know everything yet? I find the MOND discussions interesting.

If you ever want to feel queasy about dark matter, try getting up in front of several dozen students and explaining it. Yup.

—— lisa, 7:04 PM, Thursday, October 13, 2005

What's so disconcerting about explaining to your students that 90% of the mass in the universe is something which they can't touch, can't see, and which doesn't even leave a funny smell? But that apparently all of the galaxies in the Universe would fly apart without it? Or that, after 30 years of not knowing what it is, we've now discovered that dark matter is only maybe 30% of the mass-energy budget of the Universe... the other 70% being some mysterious form of "dark energy," about which we are equally clueless? Hey... that's progress!

—— Jackie M., 9:12 PM, Thursday, October 13, 2005

First I tell the students about dark matter, then I have to bring up dark energy. It's a good thing this material gets covered at the end of the semester, or they'd never believe anything I say. :)

—— lisa, 7:24 PM, Friday, October 14, 2005

Dave - I passed this link on to my friend matt, a physics postdoc at cornell, and asked him what he htought; his response (in irc) was:
11:37 aphrael: the calculation is probably wrong. The idea you need GR to model a galaxy is pretty far fetched. Furthermore, galatic rotation curves are only one of many lines of evidence pointing to dark matter.

I don't know enough to comment one way or another, but I thought it would be useful to forward at least one dissenting view.

—— aphrael, 10:29 AM, Saturday, October 15, 2005

(Of course, you'll notice that none of us actually wants to read all of that general relativity to find the error ourselves...)

But yeah, what he said. I suspect if you can find a way to make general relativity account for galactic rotation curves, then that same calculation will also account for gravitational lensing measurements. And that's it. I doubt you'll be able to recalculate the Friedmann-Lemaitre-Robertson-Walker metric to neatly disembowel all of the corroborating cosmological evidence for dark matter (from the cosmic microwave background and structure formation models) the same way. The overall mass density in the Universe is just too high, period.

—— Jackie M., 1:36 PM, Saturday, October 15, 2005

While galactic rotation curves are only one piece of evidence for dark matter, they were the first piece of evidence. Structure formation models and CMB fluctuation measurements have been interpreted with dark matter in mind. I wonder how extragalactic astronomy would have progressed if the rotation curves had been explained differently?

I do agree that GR is overkill for the rotation curves.

—— Dr. Lisa, 5:04 PM, Saturday, October 15, 2005

Hey, but they weren't looking for dark energy, either, were they?

Yeah, the numerical simulations are all chock full of let's-just-assume-that-they're-already-there dark matter particles. But I don't think any assumption goes into the FLRW models... all that says is, the Universe will collapse or expand if the energy-mass density is respectivley above or below the critical value.

Once you glue together the supernovae measurements and the CMB, doesn't it just sorta plop right out? Omega_M = 0.3, Omega_L = 0.7. You don't even really need structure formation or nucleosynthesis anymore... but weren't they getting Omega_M = 0.3 from galaxy redshift surveys already?

They just happened to think it was problematic for the opposite reason: the theorists insisted on Omega = 1. If they hadn't know about dark matter already from rotation curves, then they would have been arguing the other way -- that there's only about Omega_M ~ 0.03's worth of baryons in the Universe, and oh no! we keep getting Omega_M = 0.3. And Omega = 1 would have just been patently ridiculous, right up to the moment when the supernovae results came in.

(David, do you want us to move this conversation off-line?)

—— Jackie M., 8:52 PM, Saturday, October 15, 2005

Offline, are you kidding? I’m a science-fiction writer. This is gold.

—— David Moles, 9:25 PM, Sunday, October 16, 2005