This may be one of the best HN comments I've ever read. Thanks for posting. I do have a question though. Probably a stupid one, as IANAP(hysicist).
Regarding this:
Now, an aside. Manhattan is not undergoing cosmic expansion. The Earth-Moon system is not expanding. Neither is our solar system to the best of our ability to measure. Our galaxy and the cluster that it's in do not appear to be expanding. Distant galaxy clusters appear to be bound together against the cosmological accelerated expansion.
Do you mean that Manhattan (and the Earth-Moon system, etc.) literally are not expanding even one smidgen, or do you mean that at that scale the expansion is just too small to (notice|measure|care about)? I ask, as I'd always interpreted "expansion" as being space itself expanding, and thought that it happened at all scales (including now that I think about it, inside of atoms, which could cause some weird stuff???). But are we saying that expansion isn't something that happens at all scales then? Eg, that only the space between galaxies (or between galaxy clusters) is expanding? If so, that makes the whole expansion issue feel even weirder than ever to me, and it felt weird enough before!
IANAP, but I've been through early courses in QM & GR. The negative value of the tensor (could be) dependent upon the local curvature, such that in the region of massive objects the tensor is 0 or positive (which means "regular" GR dominates); and, "very far away" (in the cheese), the tensor is negative, and causes expansion.
> Do you mean that Manhattan (and the Earth-Moon system, etc.) literally are not expanding even one smidgen, or do you mean that at that scale the expansion is just too small to (notice|measure|care about)?
More the former.
In General Relativity, we have several exact solutions of the Einstein Field Equations, which basically means we have a lot of standard spacetime metrics. The Schwarzschild metric for a central spherically symmetrical non-rotating mass is one. The Kerr metric, which is essentially an axisymmetric deformation of Schwarzschild is another. There are related metrics which incorporate gravitationally collapsing matter into a spacetime like these.
Many such solutions are asymptotically flat. Very roughly, the inverse square law for gravity means that at a large distance you can ignore the gravitation of a central mass (which grows more and more pointlike in gravitational behaviour with increasing distance). Eventually you're in an area where the gravitational contribution can be ignored. In the language of General Relativity you are in effectively flat spacetime. The function of distance goes asymptotically to flat. There are obvious analogies with electromagnetism: distant stars are dim and pointlike, and really distant ones can be clumped together in larger structures with their clumped-together light curves being an example of an aggregated observable. (Indeed even at the level of a single star we are aggregating lots of tiny events into one spectrum equipped with emission and absorption lines, both for close-up stars and for distant ones).
We have some procedures available that let us stitch together asymptotically flat spacetimes with a "thin shell" mathematical boundary used to translate values from one side of the stitching to another. We can thus build up our solar system as a hierarchical stitching-together of Kerr-like metrics (one for each rotating body) each of which can "meet" another at some relatively flat-space point.
We can even stitch in Kerr-like metrics into a broader spacetime. The swiss cheese cosmology approach does this, and that technique traces back to the 1930s: https://en.wikipedia.org/wiki/Einstein%E2%80%93de_Sitter_uni...
(it has of course been refined over the decades).
Careful observation of our solar system supports this hierarchical stitching method reasonably well, but only if the far regions away from bodies are asymptotically flat. If we generate almost any amount of metric expansion -- much less than \Lambda -- to the otherwise asymptotically flat areas around the Earth, the moon's orbit changes dramatically. Likewise, if we change it within our solar system, things look very different in fairly short order. The same so far holds remarkably well for larger structures that are gravitationally bound, up to galaxy clusters.
A couple of decades ago, there were good astrophysical-observation reasons to think the hierarchical "stitching" process was broken enough that either an inhomogeneous metric would be needed from the start (throwing away lots of useful symmetries). These have faded with subsequent observation.
There is still some small wiggle room that allows for things like fifth-force screening to be taken seriously, however one has to do headstands to keep Manhattan (or Earth-Moon or Earth-Sun) from expanding measurably.
Measurability here is very tight. Laser lunar ranging, very long baseline interferometry, and even GPS and friends keep tightening the bounds on how much expansion the "true" metric Earth sources can allow compared to its approximate Kerr metric.
This is why I think it is safer to say that it's not expanding at all, rather than that we will find expansion if we look closer and closer.
As a sibling comment has noted, there are also constraints from particle physics and chemistry. Those constraints also arise in astrophysical systems like megamasers, planetary nebulae, stellar deflagrations, supernovae, binary+ millisecond pulsars, and so forth. The wiggle room for a suppression rather than extinction of cosmological expansion keeps tightening, and the constraints are from a diversity of lines of evidence.
However, it is reasonable to qualify the "it's not expanding" with "all our measurements to date are consistent with exactly no expansion in the solar system, and we have lots of rather different types of measurements all saying the same thing". I'm not sure that's as helpful for understanding the physical neighbourhood around here, or in galaxies and star systems generally, though.
> I'd always interpreted "expansion" as being space itself expanding, and thought that it happened at all scales
Observations are consistent with expansion happening only in really good extragalactic (extra-galaxy-cluster, even) vacuum.
This is really easy to explain with a non-accelerating expanding universe.
The mechanism for the (actually accelerated!) expansion is not known, but is usually what is meant by "dark energy".
This is a highly conventional take on the matter. I'm not offering up any sort of pet hypotheses, and I generally avoid doing so anywhere like HN as explaining the standard theory is more interesting (even to me) anyway.
The sky is full of weird stuff that can be seen. Check out the "variable universe" -- astronomers like https://asas-sn.osu.edu/atlas/visualizations#star-map-panel keep finding bizarro things to think about even far away (in a theory-space sense) from the dark matter / dark energy sectors, that may test theories about those sectors.
You'd expect that as visible matter gets weirder, the invisible stuff must get weirder still in proportion. Oddly, that is not really the case.
Thank you, you're a fantastic writer and clearly have some expertise. I am not on your level but do spend a decent amount of time trying to deepen my understanding of physics.
This got me thinking, would one way to explain expansion possibly be gravity is slowly getting stronger on shorter distances, or that the fabric of spacetime itself is not perfectly rigid, not only in the "depth" component like the classic trampoline analogy, but also in the "length/width" component? Galaxy filaments are thinning, so if you think of the center of a supervoid surrounded by filaments on all sides, that void is being stretched apart in every direction, at some level that is so fundamental that it "creates more space". Then again, everything everywhere is surrounded by filaments and all space is being pulled apart by the same reasoning, but if there is anisotropic mass close enough, this overrides the creation of new space.
The tl;dr is that the implosion of early dense baryon clouds created shockwaves which threw most of the matter (including dark matter) out of the regions that later became cosmic voids.
Few voids are outright surrounded by denser parts of the cosmic web, and there are many "invasions" of dense filamentary structures into large voids. Additionally, at much larger scales the difference between relatively empty space and relatively full space blurs away (WiggleZ Dark Energy Survey, SDSS-BOSS) preserving our ability to work with the spatially homogeneous and isotropic distribution of matter in the concordance cosmology. Thus the matter an be modelled as a uniform "dust" whose individual motes move only with the expansion, and even as a set of perfect fluids which carry attributes such as pressure, density, velocity of sound, and effective equation of state.
It is pretty reasonable to expect that ongoing detailed sky surveys will find small numbers of galaxies and/or quasars in most voids, as any reasonably dense concentrations of matter left behind from the BAO would tend to collapse gravitationally. The orbits in such in-void structures will be important observational targets. One should expect that these galaxies (and the subsystems within them) do not expand with the cosmos any more than our galaxy or our solar system, and that their peculiar against the cosmological comoving coordinates is low, like galaxies clearly outside voids.
It seems a bit nuts that people are chasing Standard Model extensions for dark energy but they haven't even resolved particle with gravity yet, or has there been recent advances?
I never heard of string theory being somewhat formally accepted. Hm, now they have things like "loop gravity". I guess they are still trying to crack that nut.
At least we can measure gravity in a local/controlled setting...
> But are we saying that expansion isn't something that happens at all scales then? Eg, that only the space between galaxies (or between galaxy clusters) is expanding?
Yes, that's what is being said here. The space inside you and me and our atoms don't expand, but the empty spaces between galaxies do.
> Yes, that's what is being said here. The space inside you and me and our atoms don't expand, but the empty spaces between galaxies do.
It is very weird, and non-intuitive.
Why is it weird that localized entities don’t expand in the same way as galaxies do? Why would my body expand in the same way that the universe would when exposed to a Big Bang?
>(including now that I think about it, inside of atoms, which could cause some weird stuff???).
If the distance between electrons and protons were expanding over time, that would be hard to square with quantitized energy levels for electron orbitals. Not sure if you could get around having material and chemical properties changing over time.
Regarding this:
Now, an aside. Manhattan is not undergoing cosmic expansion. The Earth-Moon system is not expanding. Neither is our solar system to the best of our ability to measure. Our galaxy and the cluster that it's in do not appear to be expanding. Distant galaxy clusters appear to be bound together against the cosmological accelerated expansion.
Do you mean that Manhattan (and the Earth-Moon system, etc.) literally are not expanding even one smidgen, or do you mean that at that scale the expansion is just too small to (notice|measure|care about)? I ask, as I'd always interpreted "expansion" as being space itself expanding, and thought that it happened at all scales (including now that I think about it, inside of atoms, which could cause some weird stuff???). But are we saying that expansion isn't something that happens at all scales then? Eg, that only the space between galaxies (or between galaxy clusters) is expanding? If so, that makes the whole expansion issue feel even weirder than ever to me, and it felt weird enough before!