Good Faith

mandela-cell-jpg_extra_big Nelson Mandela was a complicated person. He was no pushover; he was an activist, a revolutionary, someone who got things done and wasn’t afraid to break a few eggs when necessary. But his greatest contribution wasn’t the overthrow of apartheid in South Africa, which arguably would have happened at some point anyway — it was the peaceful way in which the transition happened, and the inclusiveness, forgiveness, and ability to look forward with which he led the nation thereafter.

Now, the concept of “New Year’s Resolutions” is a pretty awful one. Most people resolve to lose weight or some generic version of being nicer, and most fall off the wagon pretty quickly. A health club I used to go to would display signs in January saying “Regulars: don’t worry about the crowds, most of them will be gone soon.” Not very encouraging, but pretty accurate.

But the idea of resolving to be a better person is a good one, and the beginning of a new year is as good a time as any. So without making an official resolution, this year I’d like to be more like Nelson Mandela.

Not that I’m likely to be lifting any peoples out of oppression or anything so grandiose. My personal stakes are quite a bit lower. But we live in a world where people are constantly disagreeing with each other, taking opposite sides on various issues. And disagreement about important things should be engaged in vociferously; some positions are simply wrong, and sometimes they are wrong in harmful ways. But I want to make more of an effort to treat people I disagree with as fellow human beings, not simply as opponents or enemies. When disagreement occurs, I want to start as much as possible from a position of interpretive charity, imagining that everyone in the conversation is acting in good faith and willing to listen with an open mind. That’s not always the case, but it’s the right default assumption. And it’s one that is really hard to make. There’s an enormous predilection for equating disagreement with bad faith. I disagree with that person, so they are my enemy. It’s an attractive attitude, since I get to imagine that the defense of my beliefs is a lofty moral stance. But giving into that impulse not only sends conversations down a race to the bottom, it weakens my own position. I hold nearly all of my beliefs tentatively, subject to correction in the face of new information or better arguments. To ensure that I have the most accurate beliefs possible, it’s necessary to hear the best objections to them and take them seriously, not take the lazy way out of painting their proponents as bad people.

I have a couple of science/religion debates coming up: with Hans Halvorson at Caltech on January 23, and with William Lane Craig in New Orleans on February 21. These kinds of discussions can get intense, so it’s a good challenge to try to consistently take the high road. My goal isn’t to “win” any debates; it’s to help people understand my point of view, and hopefully even learn something myself.

It’s completely possible that I’m misconstruing what Mandela was all about; I’m no expert. But I figure if he can work with the people who kept him in prison for 27 years, I can speak respectfully with people in public and on the internet. Even if they’re totally wrong (you know who you are).

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Neutrinos From the Sky

It’s been hard to find time for blogging, but there’s one story I don’t want to let slip by before the end of the year: the observation by Ice Cube of neutrinos from beyond the Solar System.

It was my own bad sense of timing to blog about Ice Cube mere days before they announced this result — but just to mention the fun fact that they confirmed the existence of the Moon. And, like noticing the Moon, there’s a sense in which we shouldn’t be too surprised — we were pretty confident that neutrinos were in fact raining down upon us from the sky all the time. But that’s a bad attitude, because this is a big deal. It’s a new way of looking at the universe, and historically new ways of looking at the universe have always brought us surprises and new insights of one form or another.

The actual process by which Ice Cube determined that they had found cosmic neutrinos is a bit convoluted, so let’s go through it. For one thing, the detector doesn’t “see” neutrinos directly. It sees Cherenkov radiation, which is emitted when a charged particle moves through a medium at a speed faster than the velocity of light in that medium. (Nothing moves faster than light moves in vacuum, but the speed of light in ice is lower than in vacuum.) Neutrinos, you may have figured from the name, are neutral particles, not charged ones. So what you’re actually seeing are events where a neutrino bumps into one of the water molecules in the ice and creates some charged particles.

But most of the neutrinos you detect by this method are not really cosmic. They’re byproducts of cosmic rays — mostly charged particles flying through space at enormous energies, which smash into Earth’s atmosphere, creating neutrinos (and various other particles) along the way. So a cosmic ray interacts with the atmosphere, creating a neutrino, which then interacts with the ice to make charged particles we can observe. Ice Cube sees these “atmospheric neutrinos” all the time; indeed, it makes maps of them. And that’s great, and certainly helps teach us something about cosmic rays. But it would still be cool to find some neutrinos that have themselves made the long journey across the desolate cold of interstellar space. And that’s not easy; even if the detector finds some, they are likely to be swamped by the bountiful atmospheric beasts.

Enter Bert and Ernie.

Bert-and-ernie

Those are the colorful names given to two events observed over the last couple of years by Ice Cube. What makes them remarkable is their very high energies; over 30 trillion electron volts (TeV). (Francis Halzen, doyen of the experiment, “takes no responsibility” for the whimsical names.) That’s a lot more than you would expect from atmospheric neutrinos, but right in line for the most energetic cosmic neutrinos we predicted. But it’s only two events; the finding was announced earlier this year, but like good cautious scientists the collaboration didn’t quite say they were sure the events were cosmic in origin. (Note that a “cosmic neutrino” is one that traveled across the cosmos by itself, not one that was produced by a cosmic ray — sorry for the confusing nomenclature, it’s a cosmic world out there.)

Now we can do better. In November, right after my blog post about the Moon, Ice Cube announced that they had more data, and were able to identify another twenty-six events at very high energies. They put the confidence that these are truly cosmic neutrinos at four sigma — perhaps not quite the five-sigma gold standard we would like to reach, but pretty darn convincing (especially where anything astrophysical is concerned).

This result opens up a new era in astronomy. We can now look at the universe with neutrino eyes. Previously we had discovered neutrinos from the Sun, as well as the lucky few from Supernova 1987A, but now we apparently have a persistent source of these elusive particles from very far away. Perhaps from the center of our galaxy, or perhaps from hyper-energetic events in galaxies well outside our own. At the very least this kind of work should teach us something about the origin of cosmic rays themselves, and who knows what else.

I’m not sure whether to feel happy or sorry for Bert and Ernie themselves. Born in a cosmic cataclysm half a universe away, they sped through billions of miles of empty space, witnessing untold astronomical wonders, only to come crashing into the ice on a fairly run-of-the-mill planet. But at least they brought more than a little joy to the hearts of some curious scientists, which is more than most particles can say.

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Revisiting the Moon

For the first time since 1976, an artificial vehicle has landed on on the Moon. In this case it’s China’s Chang’e-3 mission, carrying a six-wheeled rover called Yutu (“Jade Rabbit”). Emily Lakdawalla at the Planetary Society blog has made some animated gifs from the video broadcast by Chinese TV. (See below the fold.) Note that these were recorded and then played back at high speed; the rover was actually moving more slowly than portrayed here.

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Nobel Day

Today was the Nobel Prize ceremony, including of course the Physics Prize to François Englert and Peter Higgs. Congratulations once again to them!

Englert and Higgs

(Parenthetically, it’s sad that the Nobel is used to puff up national pride. In Belgium, Englert gets into the headline but not Higgs; in the UK, it’s the other way around.)

I of course had nothing to do with the physics behind this year’s Nobel, but I did write a book about it, so I’ve had a chance to do a little commentating here and there. I wrote a short piece for The Independent that tries to place the contribution in historical context. I’ve had a bit of practice by now in talking about this topic to general audiences, so consider this the distillation of the best I can do! (It’s a UK newspaper, so naturally only Higgs is mentioned in the headline.) I love how, at the bottom of the story, you can register your level of agreement, from “strongly agree” to “strongly disagree.” And if you prefer your words spoken aloud, here I am on the BBC talking about the book.

270px-Murray_Gell-Mann_-_World_Economic_Forum_Annual_Meeting_2012Meanwhile here at Caltech, we welcomed back favorite son Murray Gell-Mann (who spends his days at the Santa Fe Institute these days) for the 50th anniversary of quarks. One of the speakers, Geoffrey West, pointed out that no Nobel was awarded for the idea of quarks. Gell-Mann did of course win the Nobel in 1969, but that was “for his contributions and discoveries concerning the classification of elementary particles and their interactions”. In other words, strangeness, SU(3) flavor symmetry, the Eightfold Way, and the prediction of the Omega-minus particle. (Other things Gell-Mann helped invent: kaon mixing, the renormalization group, the sigma model for pions, color and quantum chromodynamics, the seesaw mechanism for neutrino masses, and the decoherent histories approach to quantum mechanics. He is kind of a big deal.)

But, while we now understand SU(3) flavor symmetry in terms of the quark model (the up/down/strange quarks are all light compared to the QCD scale, giving rise to an approximate symmetry), the idea of quarks itself wasn’t honored by the 1969 prize. If it had been, the prize certainly would have been shared by George Zweig, who proposed the idea independently. So there’s still time to give out the Nobel for the quark model! Perhaps Gell-Mann and Zweig could share it with Harald Fritzsch, who collaborated with Gell-Mann on the invention of color and QCD. (The fact that QCD is asymptotically free won a prize for Gross, Politzer and Wilczek in 2004, but there hasn’t been a prize for the invention of the theory itself.) Modern particle physics has such a rich and fascinating history, we should honor it as accurately as possible.

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The Branch We Were Sitting On

barnes_julian-19911205025R.2_png_380x600_crop_q85In the latest issue of the New York Review, Cathleen Schine reviews Levels of Life, a new book by Julian Barnes. It’s described as a three-part meditation on grief, following the death of Barnes’s wife Pat Kavanagh.

One of the things that is of no solace to Barnes (and there are many) is religion. He writes:

When we killed–or exiled–God, we also killed ourselves…. No God, no afterlife, no us. We were right to kill Him, of course, this long-standing imaginary friend of ours. And we weren’t going to get an afterlife anyway. But we sawed off the branch we were sitting on. And the view from there, from that height–even if it was only an illusion of a view–wasn’t so bad.

I can’t disagree. Atheists often proclaim the death of God in positively gleeful terms, but it’s important to recognize what was lost–a purpose in living, a natural place in the universe. The loss is not irretrievable; there is nothing that stops us from creating our own meaning even if there’s no supernatural overseer to hand one to us. But it’s a daunting task, one to which we haven’t really faced up.

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The Spark in the Park

A few years ago, not long after we moved to LA, Jennifer and I got a call from some of the writers on the TV series BONES. There’s already a science component to the show, which features brainy forensic anthropologist Brennan (Emily Deschanel) and her team of lab mates working with fiery FBI agent Booth (David Boreanaz) to solve crimes, most of which involve skeletons and physical evidence in some crucial way. This time they needed some physics input, as they wanted the murderer to be a researcher who used their physics expertise to carry out the crime, and were looking for unusual but realistic ideas. We were able to provide some crucial sociological advice (no, professional research scientists probably wouldn’t meet at a Mensa conference) and consulted with experimentalist friends who would know how to use radioactive substances in potentially lethal ways. I won’t say who, exactly, but when the episode aired they ended up calling the research institute the Collar Lab.

booth-and-bones

Apparently physicists are a suspiciously violent bunch, because tonight’s episode features another scientist suspect, this time played by Richard Schiff of West Wing fame. I got a chance to consult once again, and this time contributed something a bit more tangible to the set: a collection of blackboards in the physicist’s office. (Which, as in all Hollywood conceptions, is a lot more spacious and ornate than any real physicist’s office I’ve ever seen.) You can see the actual work tonight (8pm ET/PT on Fox), but here’s one that I made up that they didn’t end up using.

bones-board

It does look like our professor is a theoretical cosmologist of some sort, doesn’t it? The equations here will be familiar to anyone who has carefully read “Dynamical Compactification from de Sitter Space.” The boards that actually will appear on the show are taken mostly from “Attractor Solutions in Scalar-Field Cosmology” and “A Consistent Effective Theory of Long-Wavelength Cosmological Perturbations.” Hey, if I’m going to write down a bunch of equations, they might as well be my equations, right?

But I actually got to be a little more than just a technical scribe. (Although that’s not an unimportant role — not only are the equations themselves gibberish to non-experts, it’s difficult for someone who isn’t familiar with the notation to even accurately transcribe the individual symbols.) No spoilers, but the equation-laden blackboards actually play a prominent role in a scene that appears late in the episode, so I was able to provide an infinitesimally tiny amount of creative input. And the scene itself (the overall conception of which belongs to writers Emily Silver and Stephen Nathan) packs quite an emotional wallop, something not typically associated with a series of equations. I haven’t seen the finished episode yet, but it was a great experience to actually be present on set during filming and watch the sausage being made.

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Thanksgiving

This year we give thanks for an idea that establishes a direct connection between the concepts of “energy” and “information”: Landauer’s Principle. (We’ve previously given thanks for the Standard Model Lagrangian, Hubble’s Law, the Spin-Statistics Theorem, conservation of momentum, effective field theory, the error bar, and gauge symmetry.)

Landauer’s Principle states that irreversible loss of information — whether it’s erasing a notebook or swiping a computer disk — is necessarily accompanied by an increase in entropy. Charles Bennett puts it in relatively precise terms:

Any logically irreversible manipulation of information, such as the erasure of a bit or the merging of two computation paths, must be accompanied by a corresponding entropy increase in non-information bearing degrees of freedom of the information processing apparatus or its environment.

The principle captures the broad idea that “information is physical.” More specifically, it establishes a relationship between logically irreversible processes and the generation of heat. If you want to erase a single bit of information in a system at temperature T, says Landauer, you will generate an amount of heat equal to at least

(\ln 2)k T,

where k is Boltzmann’s constant.

This all might come across as a blur of buzzwords, so take a moment to appreciate what is going on. “Information” seems like a fairly abstract concept, even in a field like physics where you can’t swing a cat without hitting an abstract concept or two. We record data, take pictures, write things down, all the time — and we forget, or erase, or lose our notebooks all the time, too. Landauer’s Principle says there is a direct connection between these processes and the thermodynamic arrow of time, the increase in entropy throughout the universe. The information we possess is a precious, physical thing, and we are gradually losing it to the heat death of the cosmos under the irresistible pull of the Second Law.

The principle originated in attempts to understand Maxwell’s Demon. You’ll remember the plucky sprite who decreases the entropy of gas in a box by letting all the high-velocity molecules accumulate on one side and all the low-velocity ones on the other. Since Maxwell proposed the Demon, all right-thinking folks agreed that the entropy of the whole universe must somehow be increasing along the way, but it turned out to be really hard to pinpoint just where it was happening.

maxwellsdemon

The answer is not, as many people supposed, in the act of the Demon observing the motion of the molecules; it’s possible to make such observations in a perfectly reversible (entropy-neutral) fashion. But the Demon has to somehow keep track of what its measurements have revealed. And unless it has an infinitely big notebook, it’s going to eventually have to erase some of its records about the outcomes of those measurements — and that’s the truly irreversible process. This was the insight of Rolf Landauer in the 1960’s, which led to his principle.

A 1982 paper by Bennett provides a nice illustration of the principle in action, based on Szilard’s Engine. Short version of the argument: imagine you have a piston with a single molecule in it, rattling back and forth. If you don’t know where it is, you can’t extract any energy from it. But if you measure the position of the molecule, you could quickly stick in a piston on the side where the molecule is not, then let the molecule bump into your piston and extract energy. The amount you get out is (ln 2)kT. You have “extracted work” from a system that was supposed to be at maximum entropy, in apparent violation of the Second Law. But it was important that you started in a “ready state,” not knowing where the molecule was — in a world governed by reversible laws, that’s a crucial step if you want your measurement to correspond reliably to the correct result. So to do this kind of thing repeatedly, you will have to return to that ready state — which means erasing information. That decreases your phase space, and therefore increases entropy, and generates heat. At the end of the day, that information erasure generates just as much entropy as went down when you extracted work; the Second Law is perfectly safe.

The status of Landauer’s Principle is still a bit controversial in some circles — here’s a paper by John Norton setting out the skeptical case. But modern computers are running up against the physical limits on irreversible computation established by the Principle, and experiments seem to be verifying it. Even something as abstract as “information” is ultimately part of the world of physics.

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Winton Prize

Greetings from Paris, where we just arrived from London via the technological miracle of the Chunnel. I was in London in part to take place in the award ceremony for the Royal Society Winton Prize for science books. Which, to my honest surprise, I won!

winton Not to everyone’s surprise, as it turned out. As the big moment approached, with all six short-listed authors and their friends sitting nervously in the audience, President of the Royal Society Paul Nurse took the podium to announce the winner. He played up the tension quite a bit, joking that nobody in the room, not even he, knew what name was written in the sealed envelope he held in his hands. Unbeknownst to Nurse, a slight technical glitch had caused a PowerPoint slide showing The Particle at the End of the Universe to be displayed — with the word “Winner.” So actually, he was the only one in the room who didn’t know by that point.

Other than that amusing diversion, however, it was a great event overall. It’s such a pleasure to experience the strong culture of public science that is thriving in the UK, and the Royal Society deserves a lot of credit in helping to bring science writing to a wider audience.

I wouldn’t have wanted to be on the prize jury, however. All of the six shortlisted books are fascinating in their own ways, and at some point it’s comparing apples to pears. I wouldn’t have been surprised if any of the other contenders had walked away with the trophy:

But, you know, someone has to win. I’ll admit I was rooting for me. Hearing all the congratulations from Twitter/Facebook/email etc. has been extremely heart-warming. (And yes, we’re all hoping that there’s more gender/ethnic diversity on future shortlists…)

Recognizing all the while, of course, what I owe to many other people. While writing this book I was as much of a journalist/evangelist hybrid as I was a scientist, helping to spread the word of the amazing work done by thousands of experimental physicists and technicians, and I hope that the book made their contribution more widely appreciated. Most of all, I fully appreciate that I’m not even the best writer in my own house (which only has two people in it). Jennifer is going to quickly tire of hearing me say “Who’s the award-winning author around here, anyway?”

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Scientists Confirm Existence of Moon

Bit of old news here — well, the existence of the Moon is extremely old news, but even this new result is slightly non-new. But it was new to me.

Ice Cube is a wondrously inventive way of looking at the universe. Sitting at the South Pole, the facility itself consists of strings of basketball-sized detectors reaching over two kilometers deep into the Antarctic ice. Its purpose is to detect neutrinos, which it does when a neutrino interacts with the ice to create a charged lepton (electron, muon, or tau), which in turn splashes Cherenkov radiation into the detectors. The eventual hope is to pinpoint very high-energy neutrinos coming from specific astrophysical sources.

For this purpose, it’s the muon-creating neutrinos that are your best bet; electrons scatter multiple times in the ice, while taus decay too quickly, while muons give you a nice straight line. Sadly there is a heavy background of muons that have nothing to do with neutrinos, just from cosmic rays hitting the atmosphere. Happily most of these can be dealt with by using the Earth as a shield — the best candidate neutrino events are those that hit Ice Cube by coming up through the Earth, not down from the sky.

It’s important in this game to make sure your detector is really “pointing” where you think it is. (Ice Cube doesn’t move, of course; the detectors find tracks in the ice, from which a direction is reconstructed.) So it would be nice to have a source of muons to check against. Sadly, there is no such source in the sky. Happily, there is an anti-source — the shadow of the Moon.

Cosmic rays rain down on the Earth, creating muons as they hit the atmosphere, but we expect a deficit of cosmic rays in the direction of the Moon, which gets in the way. And indeed, here is the map constructed by Ice Cube of the muon flux in the vicinity of the Moon’s position in the sky.

moon-icecube

There it is! I can definitely make out the Moon.

Really this is a cosmic-ray eclipse, I suppose. We can also detect the Moon in gamma rays, and the Sun in neutrinos. It’s exciting to be living at a time when technological progress is helping us overcome the relative poverty of our biological senses.

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Why Does Dark Energy Make the Universe Accelerate?

Peter Coles has issued a challenge: explain why dark energy makes the universe accelerate in terms that are understandable to non-scientists. This is a pet peeve of mine — any number of fellow cosmologists will recall me haranguing them about it over coffee at conferences — but I’m not sure I’ve ever blogged about it directly, so here goes. In three parts: the wrong way, the right way, and the math.

The Wrong Way

Ordinary matter acts to slow down the expansion of the universe. That makes intuitive sense, because the matter is exerting a gravitational force, acting to pull things together. So why does dark energy seem to push things apart?

The usual (wrong) way to explain this is to point out that dark energy has “negative pressure.” The kind of pressure we are most familiar with, in a balloon or an inflated tire, pushing out on the membrane enclosing it. But negative pressure — tension — is more like a stretched string or rubber band, pulling in rather than pushing out. And dark energy has negative pressure, so that makes the universe accelerate.

If the kindly cosmologist is both lazy and fortunate, that little bit of word salad will suffice. But it makes no sense at all, as Peter points out. Why do we go through all the conceptual effort of explaining that negative pressure corresponds to a pull, and then quickly mumble that this accounts for why galaxies are pushed apart?

So the slightly more careful cosmologist has to explain that the direct action of this negative pressure is completely impotent, because it’s equal in all directions and cancels out. (That’s a bit of a lie as well, of course; it’s really because you don’t interact directly with the dark energy, so you don’t feel pressure of any sort, but admitting that runs the risk of making it all seem even more confusing.) What matters, according to this line of fast talk, is the gravitational effect of the negative pressure. And in Einstein’s general relativity, unlike Newtonian gravity, both the pressure and the energy contribute to the force of gravity. The negative pressure associated with dark energy is so large that it overcomes the positive (attractive) impulse of the energy itself, so the net effect is a push rather than a pull.

This explanation isn’t wrong; it does track the actual equations. But it’s not the slightest bit of help in bringing people to any real understanding. It simply replaces one question (why does dark energy cause acceleration?) with two facts that need to be taken on faith (dark energy has negative pressure, and gravity is sourced by a sum of energy and pressure). The listener goes away with, at best, the impression that something profound has just happened rather than any actual understanding.

The Right Way

The right way is to not mention pressure at all, positive or negative. For cosmological dynamics, the relevant fact about dark energy isn’t its pressure, it’s that it’s persistent. It doesn’t dilute away as the universe expands. And this is even a fact that can be explained, by saying that dark energy isn’t a collection of particles growing less dense as space expands, but instead is (according to our simplest and best models) a feature of space itself. The amount of dark energy is constant throughout both space and time: about one hundred-millionth of an erg per cubic centimeter. It doesn’t dilute away, even as space expands.

Given that, all you need to accept is that Einstein’s formulation of gravity says “the curvature of spacetime is proportional to the amount of stuff within it.” (The technical version of “curvature of spacetime” is the Einstein tensor, and the technical version of “stuff” is the energy-momentum tensor.) In the case of an expanding universe, the manifestation of spacetime curvature is simply the fact that space is expanding. (There can also be spatial curvature, but that seems negligible in the real world, so why complicate things.)

So: the density of dark energy is constant, which means the curvature of spacetime is constant, which means that the universe expands at a fixed rate.

The tricky part is explaining why “expanding at a fixed rate” means “accelerating.” But this is a subtlety worth clarifying, as it helps distinguish between the expansion of the universe and the speed of a physical object like a moving car, and perhaps will help someone down the road not get confused about the universe “expanding faster than light.” (A confusion which many trained cosmologists who really should know better continue to fall into.)

The point is that the expansion rate of the universe is not a speed. It’s a timescale — the time it takes the universe to double in size (or expand by one percent, or whatever, depending on your conventions). It couldn’t possibly be a speed, because the apparent velocity of distant galaxies is not a constant number, it’s proportional to their distance. When we say “the expansion rate of the universe is a constant,” we mean it takes a fixed amount of time for the universe to double in size. So if we look at any one particular galaxy, in roughly ten billion years it will be twice as far away; in twenty billion years (twice that time) it will be four times as far away; in thirty billion years it will be eight times that far away, and so on. It’s accelerating away from us, exponentially. “Constant expansion rate” implies “accelerated motion away from us” for individual objects.

There’s absolutely no reason why a non-scientist shouldn’t be able to follow why dark energy makes the universe accelerate, given just a bit of willingness to think about it. Dark energy is persistent, which imparts a constant impulse to the expansion of the universe, which makes galaxies accelerate away. No negative pressures, no double-talk.

The Math

So why are people tempted to talk about negative pressure? As Peter says, there is an equation for the second derivative (roughly, the acceleration) of the universe, which looks like this:

\frac{\ddot a}{a} = -\frac{4\pi G}{3}(\rho + 3p) .

(I use a for the scale factor rather than R, and sensibly set c=1.) Here, ρ is the energy density and p is the pressure. To get acceleration, you want the second derivative to be positive, and there’s a minus sign outside the right-hand side, so we want (ρ + 3p) to be negative. The data say the dark energy density is positive, so a negative pressure is just the trick.

But, while that’s a perfectly good equation — the “second Friedmann equation” — it’s not the one anyone actually uses to solve for the evolution of the universe. It’s much nicer to use the first Friedmann equation, which involves the first derivative of the scale factor rather than its second derivative (spatial curvature set to zero for convenience):

H^2 \equiv \left(\frac{\dot a}{a}\right)^2 = \frac{8\pi G}{3} \rho.

Here H is the Hubble parameter, which is what we mean when we say “the expansion rate.” You notice a couple of nice things about this equation. First, the pressure doesn’t appear. The expansion rate is simply driven by the energy density ρ. It’s completely consistent with the first equation, as they are related to each other by an equation that encodes energy-momentum conservation, and the pressure does make an appearance there. Second, a constant energy density straightforwardly implies a constant expansion rate H. So no problem at all: a persistent source of energy causes the universe to accelerate.

Banning “negative pressure” from popular expositions of cosmology would be a great step forward. It’s a legitimate scientific concept, but is more often employed to give the illusion of understanding rather than any actual insight.

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