Gaia measured a billion stars and found the Milky Way's outer rotation curve falling with a fitted slope of 0.47 ± 0.15. Dark matter expected flat. MOND expected flat. The interesting question is not which camp lost. It is why both were expecting the wrong curve.
I build telescopes that map the early universe and look for cracks in relativity. This one is a crack in our own galaxy.
We cover: why being inside the Milky Way makes it the hardest galaxy in the sky to measure, what asymmetric drift quietly does to every outer data point, why the 260 billion solar mass figure is a model talking and not the stars, the equation at the heart of MOND that contains no radius at all, and the possibility that the outer disc has simply been hit too hard to tell us anything.
A Keplerian decline would not kill MOND. It would make the external field effect do a great deal of unpaid work.
CHAPTERS 00:00 Two solutions. One problem. Neither wins. 02:12 The curve Vera Rubin was not supposed to find 03:18 We're inside the galaxy. That's the problem. 04:24 The wobble that biases every outer star 05:04 What Gaia DR3 actually shows 06:34 The mass nobody actually measured 08:04 MOND: no radius, no problem. Until now. 08:56 Gaia may be saying both sides are wrong 09:24 Flaws lead to new laws 10:22 Our galaxy had a close encounter 12:28 Three stories, one curve 12:42 Dark matter adjusts. MOND adjusts. But is that enough? 13:14 The tracers that could break the tie 14:04 Are we expecting the wrong curve?
The paper that inspired this video, by Alessandro Melchiorri and Ruchika, August 2026 preprint: https://arxiv.org/pdf/2608.10189 See below for more!
Get the transcript, fascinating bonus content, and my Monday M.A.G.I.C. Message: https://briankeating.com/yt
Support Into the Impossible on Patreon, get my weekly M.A.G.I.C. Message, unfiltered bonus content, and live monthly Office Hours with me: https://www.patreon.com/drbriankeating
~545 characters out. Cuts: the asymmetric-drift mechanism detail (most technical, least load-bearing for a description), the first-principles inventory, and redundant qualifiers. Every number and attribution survives intact.
``` THE PAPER THIS VIDEO IS BUILT ON
"The Rotation Curve of the Milky Way: State of the Art, the Keplerian Decline Debate, and Implications for Dark Matter" by Alessandro Melchiorri & Ruchika (Salamanca)
A review, not a new measurement, and that is why it is useful: the authors rebuild the argument from first principles, then audit the claim everyone is fighting about.
That claim is Jiao et al. 2023. A power-law fit beyond 19 kpc gives an index of 0.47 ± 0.15, consistent with Keplerian at 1 sigma, excluding a flat curve at 3 sigma. Taken literally, the Milky Way weighs roughly 2 x 10^11 solar masses, three to five times below pre-Gaia estimates.
Melchiorri and Ruchika run their own check: an MCMC fit and a Gaussian Process reconstruction over 35 compiled measurements. The decline survives both. Their spherical-equivalent mass inside 30 kpc is 2.6 x 10^11 solar masses, 25 percent short of the flat-curve value.
Then they take it apart. Asymmetric drift alone is not the villain. The damage is correlated bias: the same tracer gradients feed both the drift correction and the pressure-support term, so a wrong tracer profile corrupts both. FIRE-2 simulations show biases of 10 to 40 km/s at 20 to 25 kpc, the size of the entire claimed decline.
Three scenarios survive: 1. The decline is real & streams, globular clusters, satellites, and the timing argument are all biased the same way. 2. The decline is real but amplified by Jeans systematics, true virial mass 5 to 8 x 10^11 solar masses. 3. The decline is an artefact and the true curve is nearly flat out to 30 kpc.
The sharpest problem is not in the error budget. Bariego-Quintana and Llanes-Estrada ran the same pipeline across all 175 SPARC galaxies and found no Keplerian taper anywhere. Run it on the Milky Way and the decline is unmistakable. Either our galaxy is exceptional, or we are measuring it in a way we cannot apply to anything else. Gaia DR4 arrives 2 December 2026.
AI Generated·May contain errors
Video Summary
AI Generated
New data from the Gaia spacecraft suggests the Milky Way's rotation curve may decline at its outer edges. This \"Keplerian decline\" challenges the dark matter paradigm and MOND, both of which typically predict flat curves. The findings raise questions about the distribution of galactic mass and whether current gravitational models or assumptions about galactic equilibrium are flawed.
For 50 years, dark matter explained why galaxies spin too fast.
Its rival, MOND, explained the same thing, with no new particles at all.
New data from a European spacecraft suggests both of them predicted the wrong curve.
I'm Brian Keating. I build telescopes that map the early universe
and monitor distant astronomical objects for signs of cracks in relativity.
400 years ago, Johannes Kepler worked out how fast a planet should orbit.
The farther out you go, the slower it moves. Galaxies refused to do that.
Dark matter was one answer. Modifying Newton's equations was the other.
Then Gaia measured a billion stars in our own galaxy, and the number
it got back was the one nobody expected.
So, start with Kepler. The solar system gave him the familiar picture.
Mercury moves much faster than Earth, and Earth moves much faster than Jupiter.
Neptune moves at the urgency of a teenager that you've asked to empty the dishwasher.
The farther away you get from the sun, the slower it orbits. Not directly proportional,
but actually proportional to 1 over the square root of the radius from the sun.
Good old Johannes worked this out over four centuries ago.
Now, Kepler had three laws. For a circular orbit, which most of the planets nearly follow,
the speed that the planet orbits is determined by the gravitating matter enclosed within that orbit.
In fact, the equation is circular speed squared equals Newton's constant times
the enclosed mass divided by a radius. Newton actually proved mathematically
why Kepler's laws are correct. Measure an orbital speed, and after assuming a geometry,
basically circular, you can infer the gravitational force that's pulling on the orbiting planet.
If the enclosed mass within the orbital radius stops increasing, the radius in the denominator
keeps growing, but the numerator stays nearly fixed. Therefore, the speed must fall.
Now, let's replace the sun with a galaxy containing only its visible gas and stars.
Far outside the bright disc, almost all of that baryonic mass is entirely enclosed.
The mass term becomes approximately constant, so the predicted velocity falls off like 1 over
the square root of radius. And, we've seen that far, far out in many galaxies.
Now, here on the slide, the gray curve is the visible matter only prediction.
If galaxies behaved like enlarged solar systems, with all of the mass essentially being
at the center, that would be the end of the story. The universe, though, has other plans,
and a larger budget for the invisible accounting that dark matter seems to require.
What astronomers actually found, dating back to Vera Rubin and her collaborators,
was the blue curve. The outer velocity remains approximately constant.
And if circular speed stays constant while radius increases,
the enclosed gravitating mass must keep increasing in roughly proportion to the radius.
The luminosity of the galaxy fades away, but the gravitational influence does not.
And that mismatch is one of the clearest reasons dark matter became central to modern astrophysics.
It's not the only reason. And it's not merely that galaxies spin too fast,
it's that their radial pattern of motion implies more gravitating mass at larger radii than the
visible mass can provide. Flat rotation curves map where the missing gravity appears to live.
The standard explanation surrounds the visible disk with a much larger dark matter halo.
The halo contributes little light, but it keeps adding enclosed mass as we move outward.
Combine the disk with the halo and the rotation curve can remain essentially flat.
That's what was observed. So where is the extra gravity coming from?
These questions are not exactly identical, but there is some commonality between them,
and the rotation curve addresses the second one, the extra gravity.
Now measuring our galaxy has one disadvantage. We're inside of it.
This beach ball shows the perspective of God outside of it, but we're inside of it looking out.
So it's like trying to infer the shape of a football stadium from inside the bleachers.
Gaia gave us these exquisite measurements of stellar positions and their motions.
But Gaia doesn't provide a button labeled the true milky way rotation curve. Click here.
That was easy.
So we have to begin with proxies. We measure stellar positions and their velocities.
We correct for their distances. It's really good. Gaia's capable of doing that.
We have to choose a model and correct for the asymmetric drift of stars that add peculiar
effects. And we have to assume something about the equilibrium and symmetry of the physics of
the problem. And then we can correct for a circular velocity and any biases that we may
have induced. The instrument, Gaia, provides the data, and the pipeline tells us what we
think those data points mean. Revolutionary claims need us to keep those chapters together.
And one of the most important things is that stars do not travel on perfectly circular tracks,
just like planets. They're not perfectly ellipticity free, but they also have wobbles.
They wobble radially and vertically. And stellar populations average azimuthal speed is therefore
lower than the circular speed of the gravitational field. That difference is called by professional
astronomers asymmetric drift. Recovering the circular velocity requires a model of that
Unfortunately, the correction matters most in the outer galaxies where stars become sparse,
and that's the most important part because you have most of the enclosed mass within you
the farther out you go. And there is where the disputed decline becomes interesting.
In this analysis, the inferred speed would fall by about 30 kilometers per second between 19.5
to 26.5 kiloparsecs from the center. The fitted outer slope is negative 0.47 plus or minus 0.15.
Even though it sounds close to negative 0.5, which would be one over square root of radius,
a declining outer curve looks increasingly plausible. A precisely Keplerian decline is
more debatable. Converting it into an extraordinarily low galactic mass is more
model dependent even still. If the circular velocity really fell as one over the square root
of radius, then the velocity squared falls as one over radius. Now, if you insert that into
the circular velocity equation and the enclosed spherical equivalent mass becomes approximately
constant. You move outward but infer surprisingly little additional gravitating mass, which is
awkward for a large extended halo whose enclosed mass should keep growing. And that's a dominant
paradigm for the dark matter picture where galaxies are formed and held together and
their rotation is driven by the enclosed mass within their visible light radius.
But notice the phrase I just used, spherical equivalent. The Milky Way contains a disk,
gas, a bulge, a warp, and a three-dimensional halo. Turning one curve into a mass really
requires a lot of geometrical insight. So where do we go next? The dramatic analysis produces an
average total mass estimate of about 2.6 times 10 to the 11 solar masses. That's a lot, 260
billion equivalent solar masses. So this isn't actual stars, but it's stars, gas, and dust.
That's below many independent estimates, which are closer to a trillion solar masses. The number
comes from fitting the measured rotation curve and extending a mass model well beyond the region
directly constrained by the stars alone. So this value is very interesting, but its precision
should not hide the assumptions that produce it, as all good models have to incorporate.
The Gaian-Basin rotation curve is constrained over roughly 9 to 27 kiloparsecs. A Milky Way halo
though may extend to something like 200 kiloparsecs. So when data extending nearly 30 kiloparsecs
produce a total halo mass, most of the mass supplied by that fitted model rather than that
traced directly by the stars in that curve. Extrapolation is therefore unavoidable.
Observed and extrapolated aren't synonyms. Inside, Gaia constrains the dynamics. Outside,
we have to make theoretical choices to do most of the work.
Now at this point, when you start to hear that the paradigm of dark matter
may have failed to reproduce the dynamics, you might start to celebrate if you're a MOND advocate
like my past guest Stacey McGaugh or the founder of the MOND paradigm, Mordecai Milgrom himself.
MOND proposes that below a characteristic acceleration, the effective dynamics depart
from the Newtonian relationship. In the MOND region, the acceleration is approximately the
square root of the Newtonian acceleration times the MOND scale, which is known as A0.
For an isolated baryonic mass, this changes the expected orbital behavior without surrounding
the galaxy with a conventional particle halo. So MOND has achieved real predictive
successes at galactic scales, including the tight relationship between baryonic structure
and the observed acceleration. So if the dark matter paradigm's curve has a problem,
does MOND just win? Now this is where it becomes deliciously inconvenient for both scenarios.
How does MOND's predictions relate to what Gaia has observed?
So in this low acceleration limit required for structure to ever form and not have too
high a velocity dispersion, the velocity to the fourth power equals Newton's constant
times the baryonic masses times this constant A0, this baseline acceleration.
So what's missing from this equation? Radius. There's no radius in there.
And that's why MOND produces an asymptotically flat rotation curve for an isolated galaxy.
That was one of the great attractions, no pun intended, that Mordecai and others
were drawn in by. But now it's part of its vulnerability. It might be part of its downfall
if these data are reproducible. If the Milky Way's outer curve is Keplerian, MOND is also
expecting something flatter too, but it didn't find that. Dark matter and MOND arrive at the
flat outer rotation curves through completely different physics. Dark matter says there's
additional gravitating mass. MOND says the low acceleration dynamics are different themselves.
A robust Keplerian decline would challenge the simplest extended halo expectation,
and the deep MOND asymptotic behavior. The question becomes not which of these two camps
won, but why were both expecting the wrong curve?
So bad news for everybody is often excellent news for science. I usually say that flaws
lead to new laws. That's what I teach my students. When you find a crack, when you find something
unexpected, as Einstein did with Newton's gravity for example, and as MOND may have
done with the dark matter paradigm, and as inflation did with the big bang paradigm,
these are exciting times for scientists. A Keplerian decline would not instantly falsify
every version of MOND. MOND is nonlinear, so an external gravitational field can influence
a galaxy's internal dynamics and modify the Milky Way's outer behavior. The external
field effect can generate a decline. So the defensible conclusion is not that Gaia killed
MOND. A robust Keplerian curve would instead create tension with the isolated prediction
and require that the external gravitational field or another refinement do substantial
quantitative work. The scientific test is whether the theory fits the measured curve
with independent justified parameters, not whether or not we can tell a cool story after
seeing it. Now here's where I have to insert a warning. This is where experimentalists
like me get interested, excited, but also a little bit nervous. Distance errors will
alter both the star's inferred position and its tangential velocity. Any asymmetric
drift corrections depend on the tracer density, the gravitation field, and the velocity dispersion,
how much these stars are moving independently of the gravitational force of the dark matter
or MOND. Selection effects can change which stars enter the sample. The warp violates
simple disk geometry. Sagittarius and the Large Magellanic Cloud also drive non-circular
motion, they're like outer gravitating masses. These tracers become sparse at great distances,
and you have to question whether or not the stars are in actual equilibrium. Now,
in the Gaia analyses, neglected dynamical terms and the systematic error budget grow
towards the outermost radii, they increase, it gets harder and harder to do, and you get
more and more contamination from external gravitating masses like the LNC. None of this
proves the decline is false, by the way, it's a brilliant result. It means that the blue
curve that we showed earlier may conceal a messy galaxy. Maybe that teenager's to blame.
The more revolutionary the inference, the more carefully we have to distinguish between
what Gaia measured from what we or our proponents of MOND or dark matter would like to interpret.
Now, before you declare a winner, MOND has one more move. It isn't a linear theory,
which means a galaxy sitting inside someone else's gravitational field doesn't behave
like one sitting by itself. And the Milky Way sure ain't lonely. Now, as I said,
the Milky Way is not some isolated perfect galaxy that's relaxed in a laboratory just hanging out.
The Sagittarius dwarf galaxy nearby, but not part of our galaxy, has reportedly crossed
and perturbed our Milky Way's disk. The Large Magellanic Cloud is massive, it's nearby,
and it's dynamical, it's rotating, it's doing its own thing, too. Together with the Milky Way's
galactic warp, these interactions can produce ripples, star streams, and north-south asymmetries
between the upper and lower halves of the galaxy. These motions are valuable, but they're not
necessarily indicative of equilibrium circular motion. So you wouldn't expect Kepler's law to
actually hold in that sense. Force a disturbed population into a steady axisymmetric model,
and the reconstructive curve will absorb the disturbance and present it as a modification
to gravity. Sometimes the galaxy is telling us about dark matter, sometimes it's telling us that
it recently had a close encounter of the third kind. So where does it leave us? At this point,
there's three possibilities that I would say remain viable. First, the decline is real,
but it's moderate. The Milky Way has a lighter or more concentrated halo than some older models
suggested. Dark matter and MOND both can adjust their parameters, tune them, and survive. Second,
the decline is real, but it's exaggerated. It's affected by systematics and disequilibrium which
were implicitly assumed in the models. It's the least glamorous answer, which is why scientists
have to take it seriously. Third possibility, the outer disk is sufficiently disturbed that
the reconstructed curve can never be assumed to be equilibrium and circular and represent
the Keplerian profile at all. So we have one pattern and three possible physical stories
that explain it. The evidence that we have doesn't uniquely constrain or select between the three of
them. So what would actually settle the tie, if you will? But there are different objects we can
use. Young stars called Cepheids are dynamically colder, stellar streams can probe objects farther
out, and globular cluster satellites can test at larger radii. That's in fact how we knew the galaxy
had a certain size from the beginning with the Shapley debate of the 1920s. Future Gaia releases
improve their astrometry, the position, and velocity. We'll also get radioastronomical
surveys that will supply different tracers, typically of the gas. And better theoretical
models can include the warp, the Sagittarius mini dwarf galaxy effect, and the LMC's effects as well
explicitly. If we combine those methods with different assumptions and different systematics,
and we recover the same decline, then we'll have to listen. It'll go from three sigma to many,
many sigma in that case, potentially. But our galaxy may be asking a nastier question.
Not did dark matter lose, not did MOND win, but rather, are we expecting the wrong curve?
So what do you think is more preferable, given the evidence we've presented today?
MOND, dark matter, or something else entirely? Leave your comment below, give the video a thumbs
up, exercise your thumb, and don't forget to share this like invisible dark matter
throughout your own universe. I'm Brian Keating, Chancellor Distinguished Professor
of Physics at the University of California, San Diego, and I'll see you next time on the channel.
And I'd like to conclude this video by thanking my good friend Alessandro Melchiorri
and his collaborator, Ruchiko. They produced the paper that inspired this. It came out in August.
It's still a preprint, but it's called The Rotation Curve of the Milky Way, State of the Art,
The Keplerian Decline Debate, and Implications for Dark Matter. It's a brilliant paper,
and anyone can understand it. They summarize the field, the history, and the controversy,
so make sure you check that out. I'll leave a link in the description below.
Kepler said that the outer stars should slow down. For 50 years, our galaxy said otherwise,
and we invented an invisible halo to explain it. Now, our galaxy may be taking it back.
If that changes how you think about what we actually know, subscribe and tell me which
one you prefer. And don't forget to watch my interviews with Stacey McGaw and with Mordecai
Milgram.