Roger Penrose won the Nobel Prize for showing that black holes are an almost-unavoidable prediction of classical general relativity. Let's take a peek into what that entailed. 1/n
Einstein wrote down the equation for the dynamics of spacetime in 1915. It was complicated, and he was skeptical that it could be solved exactly. For his own investigation of e.g. the orbit of Mercury, he used approximation methods like any good physicist. 2/
But just a month later Karl Schwarzschild, taking time off between battles in the German army, found an exact solution under the assumption of perfect spherical symmetry. Tragically, Schwarzshild died of pemphigus a year later. 3/
Schwarzschild's solution gives the metric tensor - a mathematical way of expressing the geometry of spacetime. But at certain locations the metric seemed to become infinitely big - a singularity. What was up with that? 4/
Eventually physicists understood that one of the supposed singularities, at the "Schwarzschild Radius" r = 2GM, was just a mathematical artifact, and was absent in better coordinate systems. We now know this radius defines the event horizon of a black hole. 5/
Once anything falls inside the event horizon, it can never escape back to the outside world (according to classical general relativity). To do so would require moving faster than light, which is a no-no. 6/
But another singularity, at r = 0, was more serious. It represents a true blowing-up of the physical curvature of spacetime. General relativity seems to predict that general relativity itself starts to fail at this singularity. Or something. 7/
Maybe there is no physical way to make black holes? But in 1939 Robert Oppenheimer and Harlan Snyder showed that matter could collapse beyond the event horizon, apparently creating a black hole. 8/
Aside: "r" is the radial coordinate, the distance from the center. But spacetime is tricky, and inside the Schwarzschild radius the r coordinate points along time, not in a direction of space. r=0 isn't the center of the black hole, it's in the *future*. 9/
Anyway: one might guess that the r=0 singularity was a different kind of mathematical artifact, arising from the initial assumption of perfect spherical symmetry. That's what Penrose disproved; singularities are inevitable in certain circumstances. 10/
He built on a fundamental result by Amal Raychaudhuri and Lev Landau. They (independently) showed how to characterize the focusing and twisting of a group of nearby particles floating through spacetime. en.wikipedia.org/wiki/Raychaudh… 11/
Gravity is attractive. The Raychaudhuri equation shows that a group of particles initially at rest with respect to each other will come together, and eventually their paths will cross. The first baby singularity theorem (though not a worrisome infinite-curvature singularity). 12/
Penrose's breakthrough (grossly simplified!) was to level-up differential geometry, the study of curvature at local points in spacetime, to differential *topology* - global properties of the manifold that are implied by that curvature. 13/
In particular he defined a "closed trapped surface" - a spherical region in space with the property that its area would decrease in any future direction, no matter how it evolved. Why? Because spacetime itself was collapsing. 14/
Then he showed (1965), using Raychaudhuri-like reasoning, that whenever you had a closed trapped surface, some future-pointing trajectories would be "incomplete." A fancy way of saying "they would hit a singularity." 15/
Basically Penrose eliminated the need for simplifying assumptions like spherical symmetry by surrounding regions of space in an inescapable mathematical cage, with nowhere to go but to collapse to a singular point. 16/
Soon thereafter, Stephen Hawking would make his bones by playing Penrose's movie backwards, showing that classical GR also predicts a singularity in the past, at the moment of the Big Bang. 17/
Singularities probably aren't physically real; they're a reminder that a classical theory like GR will break down under extreme circumstances. Hopefully quantum gravity comes to save the day, but details are sketchy at this point. 18/
Penrose has gone on to do many other cool things, as this excerpt from his Wikipedia page shows. One of the most creative mathematical physicists of the last century. 19/19
I firmly believe that the best response to speech that one disagrees with is to offer better arguments in refutation, not to silence people. But an open letter like this one in Harper's is pretty unpersuasive, to the point of being anti-productive. (1/n) harpers.org/a-letter-on-ju…
In part that's due to the particular group of signatories. Several of them are people I enormously admire. But others have themselves been involved in attempts to silence people they disagree with. And none of them is exactly lacking ways to have their voices be heard. (2/n)
More importantly, the letter declines to engage with substance, instead straw-manning the incidents they object to. We are told, for example, that "professors are investigated for quoting works of literature in class." (3/n)
Our experience constitutes only a tiny sliver of reality — me on PBS @NewsHour.
@NewsHour It’s fair to ask how we would ever know something like that. The answer is that we provisionally accept the best theory we have that explains what we do experience, and if that implies there’s much more out there, so bit it.
Of course someone might come up with a better theory, or new data might change our view of the best current one. But until then, the universe is under no obligation to confine its extent to that which is easily perceptible to us.
One of the many great things about Pi is that it's algorithmically compressible. You can express the idea of Pi using far fewer characters than are actually contained in its numerical expression (which would be an infinite number). #PiDay 1/
Between 0 and 10 (say), there are an infinite number of rational numbers: those expressible as p/q, where both p and q are integers. The rationals are "dense" - given any number between 0 and 10, there is a rational number arbitrarily close to it. 2/
But there are infinitely more irrational numbers, those that can't be expressed as p/q. It's a bigger infinity than the number of rationals. The rationals are "countable," the irrationals are "uncountable." There are a lot of irrational numbers out there. 3/
A new study in @nature shows that small scientific teams are more likely to be truly disruptive than large collaborations. It's great work, but has engendered a "shift funding to smaller science" narrative that I think is a bit off the mark. nature.com/articles/s4158…
For one thing, I would bet that papers with fewer authors are also more likely to be ignored and get zero citations than those from big collaborations. There's just more variance in the world of papers with one or two authors.
More importantly, this paragraph in @edyong209's writeup of the story kind of undoes the narrative entirely. The causal factor doesn't seem to be size of the collaboration, it's receiving funding from top agencies! theatlantic.com/science/archiv…
Hey we have a book cover. Soon there will be an Amazon page. By September there will actually be a book you can buy! #somethingdeeply
Most of Something Deeply Hidden is about quantum mechanics generally, and Many-Worlds in particular. But the last section uses these ideas in the context of quantum gravity. Thus "Emergence of Spacetime" in the subtitle. #somethingdeeply
Quantum gravity was a big original motivation for Hugh Everett to develop the Many-Worlds approach. When there aren't observers, it's hard to make sense of the Copenhagen interpretation.
A good overview of the status of inflationary cosmology in the wake of the @Planck satellite observations, by Chowdhury, Martin, Ringeval, and Vennin. I do have one nontrivial objection... 1/n arxiv.org/abs/1902.03951
They discuss whether early inhomogeneities could prevent inflation, and conclude that the issue is open. It's not! It's perfectly clear that most inhomogeneous initial conditions, by any sensible measure, do not lead to inflation. 2/n
There are many arguments for this, the simplest of which is that you wouldn't expect a collapsing universe to anti-inflate. It's a reflection of the fact that the early universe had low entropy, which is automatically "unlikely". 3/n