Of Particular Significance

Author: Matt Strassler

Media absurdity has reached new levels of darkness with the announcement that Stephen Hawking has a new theory in which black holes do not exist after all.

No, he doesn’t.

[Note added: click here for my new introduction to the black hole information paradox.]

First, Hawking does not have a new theory… at least not one he’s presented. You can look at his paper here — two pages (pdf), a short commentary that he gave to experts in August 2013 and wrote up as a little document — and you can see it has no equations at all. That means it doesn’t qualify as a theory. “Theory”, in physics, means: a set of equations that can be used to make predictions for physical processes in a real or imaginary world. When we talk about Einstein’s theory of relativity, we’re talking about equations. Compare just the look and feel of Hawking’s recent note to Einstein’s 1905 paper on the theory of special relativity, or to Hawking’s most famous 1975 paper on black holes; you can easily see the difference without understanding the content of the papers.

The word “theory” does not mean “speculations” or “ideas”, which is all that is contained in this little article. Maybe that’s what theory means at a cocktail party, but it’s not what “theory” means in physics.

Second, what Hawking is addressing in this note is the precise level of blackness of a black hole… in short, whether the name “black hole” for the objects we call black holes is really appropriate. But simply the fact that black holes aren’t quite black isn’t new. In fact it was Hawking himself who became famous in 1974-1975 for pointing out that in a world with quantum physics, typical black holes cannot be precisely black — so it’s not true that nothing ever comes out of a black hole. Black holes must slowly radiate elementary particles, a process we call Hawking radiation.

From day 1, Hawking’s observation posed puzzles about how conflicting requirements of quantum theory and Einstein’s gravity would be resolved, with quantum theory demanding that all information that fell into the black hole be neither destroyed nor copied, and Einstein’s gravity insisting that there is no way that the information of what went into a black hole can ever come out again, even if the black hole evaporates and disappears. The assumption of the community has long been that the 1970s calculation that Hawking did, while largely correct, leaves out a small, subtle effect that resolves the puzzle. The question is: what is the nature of that subtle effect?

No one, including Hawking, has posed a satisfactory answer. And that is why we keep hearing about black holes again and again over the decades, most recently in the context of the “firewall paradox”. In his recent paper, Hawking, like many of his colleagues, is proposing another possible answer, though without demonstrating mathematically that his proposal is correct.

But did Hawking really say “There are no black holes”, or didn’t he??

Talk about taking things out of context!!! Here’s what Hawking actually said.

First he suggests that the edge of a black hole — called its “event horizon”, a very subtle concept when you get into the details — really isn’t so sharp once quantum effects are considered. Many people have suggested one version or another of this possibility, which would represent a small but critical correction to what Hawking said in the 1970s (and to what people understood about black holes even earlier).

And then Hawking writes…

“The absence of event horizons mean that there are no black holes – in the sense of regimes from which light can’t escape to infinity.”

Notice the final clause, which is omitted from the media reports, and is absolutely necessary to make sense of his remark. What he means is that black holes are very, very slightly (though importantly) less black than he said in his 1974 paper… because the things that fall into the black hole do in some sense eventually come back out as the black hole evaporates. I say “in some sense” because they come out thoroughly scrambled; you, for example, if you fell in, would not come back out, even though some of the elementary particles out of which you are made might eventually do so.

And then he says

“There are however apparent horizons which persist for a period of time.”

Translation: for an extremely long time, what we call a black hole will behave in just the way we have long thought it does. In particular, there is no change in any of the astrophysics of black holes that astronomers have been studying in recent decades. The only issue is what happens as a black hole begins to evaporate in a serious way, and when you look very, very carefully at the details of the Hawking radiation, which is very difficult to do.

“This suggests that black holes should be redefined as metastable bound states of the gravitational field.”

In short: In Hawking’s proposal, it’s not that the objects that you and I would call “black holes” don’t exist!  They are still there, just with a new name, doing what we’ve been taught they do except in some fine-grained detail. Not that this fine-grained detail is unimportant — it’s essential to resolving the quantum vs. gravity puzzle.  But an ordinary person watching or exploring near a black hole would notice no difference.

Notice also all of this is a proposal, made in words; he has not shown this with mathematics.

In short, although Hawking is, with many of his colleagues, working hard to resolve the puzzles that seem to make quantum theory conflict with Einstein’s theory of gravity in this context, he’s not questioning whether black holes exist in the sense that you and I would mean it. He’s addressing the technical issue of exactly how black they are, and how the information contained in the things that fall in comes back out again. And since he’s just got words, but not math, to back up his suggestions, he’s not convinced his colleagues.

Meanwhile, the media takes the five words “There Are No Black Holes” and creates almost pure fiction, fiction that has almost nothing to do with the reality of the science. Well done, media, well done. Sometimes you’re just like a black hole: information comes in, and after being completely scrambled beyond recognition, comes back out again through a mysterious process that makes no sense to anyone. Except that in your case, it’s very clear that information is lost, and misinformation is created.

Hey! That’s a new theory of black holes! (I’ll write a 2-page paper on that this afternoon…)

Picture of POSTED BY Matt Strassler

POSTED BY Matt Strassler

ON January 30, 2014

While the eastern half of the United States is having a cold winter so far, the same has not been true in Italy. The days I spent teaching in Florence (Firenze), at the Galileo Galilei Institute (GGI), were somewhat warmer than is apparently the usual, with even low temperatures far above freezing almost every night. A couple of people there said to me that they “hadn’t seen any winter yet”. So I was amused to read, on U.S. news websites, yet more reports of Americans uselessly debating the climate change issue — as though either the recent cold in the eastern U.S. or the recent warmth in Europe can tell us anything relevant to that discussion. (Here’s why it can’t.) It does seem to be widely forgotten in the United States that our country occupies only about 2% percent of the area of the Earth.

Of course the warmer Italian weather made my visit more pleasant, especially since the GGI is 20 minutes up a long hill — the Arcetri hill, of particular significance in scientific history. [I am grateful to the GGI, and the scientist- organizers of the school at which I taught, especially Stefania de Curtis, for making my visit to Arcetri and its sites possible.] The University of Florence used to be located there, and there are a number of astronomical observatories on the hill. And for particle physics, there is significance too. The building where I was teaching, and that hosts the GGI, used to be the department of Physics and Astronomy of the university. There, in 1925, Enrico Fermi, one of the greatest physicists of the 20th century, had his first professorial position. And while serving in that position, he figured out the statistical and thermodynamic properties of a gas made from particles that, in his honor, we now call “fermions”.  [His paper was recently translated into English by A. Zannoni.]

All particles in our world — elementary particles such as electrons and photons, and more complex objects such as atoms — are either fermions or bosons; the classic example of a fermion is an electron. The essential property of fermions is that two identical fermions cannot do precisely the same thing at the same time. For electrons in atoms, this is known as the Pauli exclusion principle (due to Wolfgang Pauli in 1925, based on 1924 research by Edmund Stoner): no two electrons can occupy the same quantum state. All of atomic physics and chemistry, and the very stability of large chunks of matter made from atoms, are dependent upon this principle. The properties of fermions also are crucial to the stability and structure of atomic nuclei, the existence of neutron stars, the electrical properties of metals and insulators, and the properties of many materials at cold temperatures.

Plaque commemorating Fermi's work on what we now call `fermions'. [Credit: M. Strassler]
Plaque commemorating Fermi’s work on what we now call `fermions’. [Credit: M. Strassler]
Inside the building is a plaque commemorating Fermi’s great achievement. But Fermi did not remain long in Florence, or even in Italy. A mere 15 years later, in the midst of the Fascist crisis and war in Europe, and having won a Nobel Prize for his work on radioactive atoms, Fermi had taken a position in the United States. There he directly oversaw the design, building and operation of humanity’s first nuclear reactor, in a secret underground laboratory at the University of Chicago, paving the way for the nuclear age.

But the main reason the Arcetri hill is famous for science is, ironically, because of a place of religion.

Both of Galileo’s daughters had taken the veil, and in 1631 the aging scientist was prompted to rent a villa on a small farm, within sight and a short walk of their nunnery.  Unfortunately, what must have seemed like an idyllic place to grow old and do science soon turned into a nightmare. After years of coexistence with and even support from within the Catholic Church, he had pushed too hard; his publication in 1632 of a comparison of the old Ptolemaic view of the universe, with the Earth at the center, with the newer Copernican view (to which he had greatly contributed, through his astronomical discoveries, in the 1610s), engendered a powerful backlash from some who viewed it as heretical. He was forced to spend 1633 defending himself in Rome and then living in exile in Sienna. When he was allowed to return to Arcetri in 1634, he was under house arrest and not allowed to have any scientific visitors. Shortly after his return, his 33-year-old daughter, with whom he was very close, died of a sudden and severe illness. His vision failed him, due to unknown diseases, and he was blind by 1638. Unable to go to Florence, his home town, scarcely three miles away, and rarely able to meet visitors, he spent the rest of his time in Arcetri isolated and increasingly ill, finally dying there in 1642.

Yet despite this, or perhaps because of it, Galileo’s science did not come to a halt. (This was also partly because of the his support from the Grand Duke of Tuscany, who interceded on his behalf to allow him some scientific assistance after he went blind.) At Arcetri, Galileo discovered the moon did not always present exactly the same face toward the Earth; it appears, to us on Earth, to wobble slightly. The explanation for this so-called “lunar libration” awaited Issac Newton’s laws of motion and of gravity, just 50 years away. And he finished formulating laws of motion (which would also later be explained by Newton), showing that (on Earth) objects tossed into the air follow a trajectory that mathematicians call a parabola, until affected by what we now call “air resistance”, and showing that uniform motion cannot be detected — the first Principle of Relativity, authored 270 years before Einstein presented his revision of Galileo’s ideas.

Vaulted ceiling in the main entry hall of Galileo's rented villa in Arcetri. (No, the light fixture is not original.) [Credit: M. Strassler]
Vaulted ceiling in the main entry hall of Galileo’s rented villa in Arcetri. (No, the light fixture is not original.) [Credit: M. Strassler]
To step into Galileo’s villa, as I did a few days ago, is therefore to step into a place of intense personal tragedy and one of great scientific achievement. One can easily imagine him writing by the window, or walking in the garden, or discussing the laws of motion with his assistants, in such a setting. It is also to be reminded that Galileo was not a poor man, thanks to his inventions and to his scientific appointments. The ceilings of the main rooms on the lower floor of the villa are high and vaulted, with attractively carved supports. There is a substantial “loggia” on the upper floor — a balcony, with pillars supporting a wooden roof, that (facing south-east, south and west) would have been ideal, while Galileo could still see, for observing the Moon and planets.

While Galileo’s luck ran badly in his later years, he had an extraordinary string of luck, as a younger scientist, at the beginning of the 1600s. First, in 1604, there was a supernova, as bright as the planet Jupiter, that appeared in the sky as a very bright new star. (Humans haven’t seen a correspondingly close and bright supernova since then, not even supernova 1987a.  There is one you can see with a small telescope right now though.) Observing that the glowing object showed no signs of parallax (see here for a description of how parallax can be used to determine the distance to an object), Galileo concluded that it must be further away than the Moon — and thus served as additional evidence that the heavens are not unchanging. Of course, what was seen was actually an exploding star, one that was nearly a trillion times further from the Earth than is the Moon — but this Galileo could not know.

Next, just a few years later, came the invention of the telescope. Hearing of this device, Galileo quickly built his own and figured out how to improve it. In the following years, armed with telescopes that could provide just 20-times magnification (typical binoculars you can buy can provide 10-times, and with much better optical quality than Galileo’s assistants could manufacture) came his great string of astronomical discoveries and co-discoveries:

  • the craters on the Moon (proving the Moon has mountains and valleys like the Earth),
  • the moons of Jupiter (proving that not everything orbits the Earth),
  • the phases of Venus and its changing apparent size as Venus moves about the sky (proving that Venus orbits the Sun),
  • the rings of Saturn (demonstrating Saturn is not merely a simple sphere),
  • sunspots (proving the sun is imperfect, changeable, and rotating),
  • and the vast number of stars in the Milky Way that aren’t visible to the naked eye.

One often hears 1905 referred to as Einstein’s miracle year, when he explained Brownian motion and calculated the size of atoms, introduced the notion of quanta of light to explain the photoelectric effect, and wrote his first two papers on special relativity. Well, one could say that Galileo had a miracle decade, most of it concentrated in 1610-1612— playing the decisive role in destroying the previously dominant Ptolemaic view of the universe, in which the Sun, Moon, planets and stars orbit in a complex system of circles-within-circles around a stationary Earth.

We live in an era where so much more is known about the basic workings of the universe, and where a simple idea or invention is rarely enough to lead to a great change in our understanding of our world and of ourselves. And so I found myself, standing in Galileo’s courtyard, feeling a moment of nostalgia for that simpler time of the 17th century, cruel and dangerous as it was… a time when a brilliant scientist could stand on the balcony of his own home, looking through a telescope he’d designed himself, and change the world-view of a civilization.

Looking across the enclosed courtyard of the villa, at the second-floor loggia, suitable for telescopic observing.  It is not hard to imagine Galileo standing there and peering into the sky.  [Credit: M. Strassler]
Looking across the enclosed courtyard of the villa, at the second-floor loggia. It is not difficult to imagine Galileo standing there and peering into his telescope. [Credit: M. Strassler]
Picture of POSTED BY Matt Strassler

POSTED BY Matt Strassler

ON January 28, 2014

As many of you have already read, there is a supernova that has gone off in a relatively nearby galaxy, and with a rather small telescope, you can see it.  And if you can find the host galaxy, M82 [often called the “cigar”, not because it is really shaped like a cigar but because it looks like one from the angle at which we see it], you can’t miss the supernova.  Like most supernovas, it’s as bright as the entire galaxy that it’s sitting in.  It will probably get a bit brighter for the next week before gradually dimming.

This supernova is of Type Ia. (There was a similar one, just a little further away, two years ago, in the galaxy M101.) This is not to be confused with a Type II supernova, in which the core of a big star, at the end of its life, runs out of fuel, collapses and explodes.  In a Type 1a, two stars, one a white dwarf (a very old star which has run out of fuel and ceased to burn, but not big enough to collapse and explode), the other a red giant (a bit younger but also old, cool and large), orbit one another.  Over time the white dwarf accumulates material from the red giant, and eventually the temperature and pressure on the white dwarf reach a critical point that causes a nuclear explosion, destroying the star in an explosion we can see well across the universe.  Or so the story goes; it’s a very plausible story, but there are details still needing clarification.

Importantly, Type Ia supernovas are quite regular (though precisely how regular is under study, and I’m sure this one will provide us with more information how about these objects work) and can therefore be used to figure out, on average, roughly how far away a host galaxy is.  This information was critical in the discovery that the universe’s expansion is accelerating rather than slowing down, i.e. in the definitive discovery of “dark `energy’ ”, also known as the cosmological constant (if it’s really in fact constant.)

M82 is about 12 million light years away, so that’s how long ago this supernova exploded; the light’s been traveling out from M82, in all directions, for 12 million years, and just reached Earth this month.  For scale, that’s about 0.1% of the age of the universe.  And it also means that this supernova is about 70 times further away than was Supernova 1987a, the bright one visible with the naked eye in the Large Magellanic Cloud (one of the satellite galaxies of our own galaxy, the Milky Way.)

A nice post which tells you more about the discovery and where to find M82 in the sky (it’s not far from the Big Dipper) can be found here.  While you’re looking, check out M81 too; no supernova there, but it’s a notable and photogenic galaxy right next to M82.

Picture of POSTED BY Matt Strassler

POSTED BY Matt Strassler

ON January 24, 2014

Last year, in a series of posts, I gave you a tour of quantum field theory, telling you some of what we understand and some of what we don’t. I still haven’t told you the role that string theory plays in quantum field theory today, but I am going to give you a brief tour of string theory before I do.

What IS String Theory? Well, what’s Particle Theory?

What is particle theory? It’s nothing other than a theory that describes how particles behave.  And in physics language, a theory is a set of equations, along with a set of rules for how the things in those equations are related to physical objects.  So a particle theory is a set of equations which can be used to make predictions for how particles will behave when they interact with one another.

Now there’s always space for confusion here, so let’s be precise about terminology.

  • “Particle theory” is the general category of the equations that can describe particles, of any type and in any combination.
  • A particle theory” is a specific example of such equations, describing a specific set of particles of specific types and interacting with each other in specific ways.

For example, there is a particle theory for electrons in atoms. But we’d need a different one for atoms with both electrons and muons, or for a bottom quark moving around a bottom anti-quark, even though the equations would be of a quite similar type.

Most particle theories that one can write down aren’t relevant (or at least don’t appear to be relevant) to the real world; they don’t describe the types of particles (electrons, quarks, etc.) that we find (so far) in our own universe.   Only certain particle theories are needed to describe aspects of our world.  The others describe imaginary particles in imaginary universes, which can be fun, or even informative, to think about.

Modern particle theory was invented in the early part of the 20th century in response to — guess what? — the discovery of particles in experiments. First the electron was discovered, in 1897; then atomic nuclei, then the proton, then the photon, then the neutrino and the neutron, and so on… Originally, the mathematics used in particle theory was called “quantum mechanics”, a set of equations that is still widely useful today. But it wasn’t complete enough to describe everything physicists knew about, even at the time. Specifically, it couldn’t describe particles that move at or near the speed of light… and so it wasn’t consistent with Einstein’s theory (i.e. his equations) of relativity.

What is Quantum Field Theory?

To fix this problem, physicists first tried to make a new version of particle theory that was consistent with relativity, but it didn’t entirely work.  However, it served as an essential building block in their gradual invention of what is called quantum field theory, described in much more detail in previous posts, starting here. (Again: the distinction between “quantum field theory” and “a quantum field theory” is that of the general versus the specific case; see this post for a more detailed discussion of the terminology.)

In quantum field theory, fields are the basic ingredients, not particles. Each field takes a value everywhere in space and time, in much the same way that the temperature of the air is something you can specify at all times and at all places in the atmosphere. And in quantum field theory, particles are ripples in these quantum fields.

More precisely, a particle is a ripple of smallest possible intensity (or “amplitude”, if you know what that means.)  For example, a photon is the dimmest possible flash of light, and we refer to it as a “particle” or “quantum” of light.

We call such a “smallest ripple” a “particle” because in some ways it behaves like a particle; it travels as a unit, and can’t be divided into pieces.  But really it is wave-like in many ways, and the word “quantum” is in some ways better, because it emphasizes that photons and electrons aren’t like particles of dust.

To sum up:

  • particles were discovered in experiments;
  • physicists invented the equations of particle theory to describe their behavior;
  • but to make those equations consistent with Einstein’s special relativity (needed to describe objects moving near or at the speed of light) they invented the equations of quantum field theory, in which particles are ripples in fields.
  • in this context the fields are more fundamental than the particles; and indeed it was eventually realized that one could (in principle) have fields without particles, while the reverse is not true in a world with Einstein’s relativity.
  • thus, quantum field theory is a more general and complete theory than particle theory; it has other features not seen in particle theory.

Now what about String Theory?

In some sense, strings also emerged from experiments — experiments on hadrons, back before we knew hadrons were made from quarks and gluons.  The details are a story I’ll tell soon and in another context. For now, suffice it to say that in the process of trying to explain some puzzling experiments, physicists were led to invent some new equations, which, after some study, were recognized to be equations describing the quantum mechanical behavior of strings, just as the equations of particle theory describe the quantum mechanical behavior of particles.  (One advantage of the string equations, however, is that they were, from the start, consistent with Einstein’s relativity.) Naturally, at that point, this class of equations was named “string theory”. (more…)

Picture of POSTED BY Matt Strassler

POSTED BY Matt Strassler

ON January 23, 2014

If you have a clear sky, don’t forget to look overhead tonight!  And go get your binoculars or small telescope…

After an overnight flight and a train that brought me to Florence (Firenze), Italy, where I’ll be teaching this week, I decided to fight off sleep by taking a walk down into the city and wandering around for a while.  It was a beautiful evening, with deep blue twilight.  And it wasn’t long before the planet Jupiter, and then the full Moon, rose above the buildings and high into the sky.  I caught a photo of them, between the Duomo (cathedral) and its campanile (bell tower).  Jupiter is the little white dot directly above the moon, at the top of the second set of windows on the campanile.

MoonJupiterOverDuomo
The Moon and Jupiter (tiny dot well above the Moon) shine between the Duomo of Florence (left) and its Campanile. Photo credit: Matt Strassler

I then pulled out my binoculars, which aren’t quite as powerful as Galileo’s telescope was 400 years ago, but are still enough to reveal what Galileo discovered.  Just as Galileo (and his competitor Thomas Herriot) did in 1609, I could see all sorts of structure to the Moon’s surface, including what we now know are basalt plains, and hints of impact craters.  [Admittedly, impact craters and mountains are actually easiest to see when the Moon isn’t full, because then the shadows that mountains cast are longer.]

And looking at Jupiter, which is relatively close to Earth right now, I could easily see that it was a disk, not a dot like a star, and that there are three dim dots, sitting in a line that passes through the planet.  These are three of Jupiter’s four large moons: Callisto, Ganymede, Europa and Io.  [The fourth one might well be visible if you’re lucky and have good eyes and good timing.]  If you watch them day by day, they will change position, a fact that Galileo used to guess they were moons orbiting Jupiter.

So if you have good weather, tonight’s a great opportunity for some simple but very satisfying astronomy.  Don’t miss the naked-eye view that’s on offer right now or in a few hours, depending on where you reside.  And if you’ve got binoculars handy, you can relive Galileo’s remarkable discoveries about the Moon and Jupiter, and contemplate how the first telescopes forever changed the way humans envisioned their cosmos.

Picture of POSTED BY Matt Strassler

POSTED BY Matt Strassler

ON January 15, 2014

Professors at research universities engage in many different activities, and one which is little known to the public involves teaching at short and focused “schools” for graduate students. These schools, which generally last one to four weeks, and are usually (but not always) held outside the main academic year in winter or summer, allow these students to learn advanced topics in short courses that their universities wouldn’t be able to offer.

For instance, at most universities in the United States, a course focused on the theory of quarks and gluons (the set of equations known as “QCD”) would be attended by just a few students. And many universities don’t even have a professor who is truly expert on this subject. But when interested students from many universities are brought together at one of these specially organized schools, a world’s expert on QCD can teach a group of students as large as fifty or more. Not only is there economy of scale in this arrangement, it also helps to foster a future community among the students who attend. I myself went to one such school when I was a graduate student, and the faculty and students I met there include a number who are my professional peers today.

Usually, professors are not paid to teach at these schools, even though preparing a course is often a huge amount of work. There are two inducements, other than the satisfaction derived from the teaching itself. The first is that travel and lodging are free for the teacher; they are paid for by the organizers of the school, who in turn get the required funds from their university and/or government organizations. The latter (wisely, in my opinion) see such schools as having national value, in that they help assure a strong national research community in the future. The second is that the schools are often held in places where a person would not regret spending a week. The schools at which I have taught over the years have occurred in Boulder, Colorado (USA); Vancouver, British Columbia (Canada); Fermilab National Lab in Aurora, Illinois (USA); Cambridge, England; Kyoto, Japan; and Varna, Bulgaria. I’ve also taught in Italy, previously in the towns of Trieste and Erice, and this month in Florence (i.e. Firenze). For the next ten days or so, I’ll be at the Galileo Galilei Institute for Theoretical Physics (GGI), which is named, of course, after Florence’s most famous scientist.

(Several of my previous short courses are available in written or video form, and most are still sufficiently up-to-date to be useful to future experts. All of them assume, at least in large part, that a student has had a beginning course in quantum field theory. I can provide some links later this week if there is interest, though most of them easily show up in a web search.)

This is my first visit to the GGI, which is associated with the University of Florence, and is located on a hill a couple of miles from downtown Florence, not very far from where Galileo himself lived for some years. It was founded around 2006 to host focused research workshops, as well as brief schools. The theoretical particle physics graduate students at this school have already learned about dark matter from Tomer Volansky (a collaborator of mine on a trigger-related project), and about supersymmetry from David Shih (a former colleague at Rutgers and a recent collaborator on a supersymmetry/LHC project.) They’ll also be learning about the Higgs phenomenon and its generalizations from Raman Sundrum (who’s been mentioned many times on this blog, and whom I visited last month); about the physics of “flavor” — including the issue of how the six different types quarks transition from one to another via the weak nuclear force — from Gino Isidori; and about the physics of quarks and gluons from one of the world’s great experts, Stefano Catani. (You may not recognize these names, as none of them have written books for the public or developed a popular website or blog; but any expert in the theoretical particle physics knows them very well.) And last and perhaps least, they’ll be learning various bits of particle physics that one ought to know in the context of particle colliders, and particularly of the Large Hadron Collider [LHC], from me.

One corollary of this news is that I’ll be pretty busy for the next ten days, so I’m not sure how active the blog will really be. But I can promise you at least one post on string theory!

Picture of POSTED BY Matt Strassler

POSTED BY Matt Strassler

ON January 15, 2014

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