Not Even Wrong

Twenty years ago this past week, John Baez posted the first of his "This Week's Finds in Mathematical Physics" to the sci.physics newsgroups, inaugurating internet blogging about Mathematical Physics, many years before anyone even knew what a blog was. For his first posting, try looking at
http://math.ucr.edu/home/baez/twf_ascii/week1
and for all the rest of them see
http://math.ucr.edu/home/baez/TWF.html

Included in his talk are various more specific comments about these issues, well worth pondering. If I were John Baez, I'd have the energy to describe them in detail and explain clearly exactly what is going on, but for this I fear someone will have to get John more interested in quantum gravity again...

Update: I should mention other tributes to TWF here, here, and here.

The University of Birmingham has put out a press release today about new research by their computer scientists, on the topic of the spread of gossip about the Higgs via Twitter. This is all based on an arXiv paper, The Anatomy of a Scientific Gossip, and has been picked up by New Scientist, Phys.org, and Aidan Randle-Conde.

Since I’ve been designated as one of the Best Physics Gossips on this topic:

If the Higgs boson was a dead celebrity, Woit would be your TMZ — first to the scene, first to break it, and have it be right.

I think I should perhaps comment on what this research actually shows. From what I can tell, it just provides evidence that Twitter is a worthless swamp full of people who have no idea what they are doing “re-tweeting” stale information to each other. Getting their information from tweets, according to these researchers things began with

Period I: Before the announcement on 2nd July, there were some rumors about the discovery of a Higgs-like boson at Tevatron;

and went on from there. They start looking at the data only from July 1 on.

Looking back at what actually happened, I started posting about the coming LHC results on June 17 (the Tevatron results were a side-show). On June 18th, Matt Strassler had the story, accusing me of ruining the CMS and ATLAS blind analyses, for top-secret reasons that could not be revealed. June 19th saw a New York Times story about this with a link to my blog entry and by June 20th Sean Carroll and Jennifer Ouellette were writing about #HiggsRumors being a “Trending Topic” on Twitter.

I suppose it’s true that a couple weeks later there were about a million tweets about this, but why would you conceivably want to look at any of them? While I was writing this blog posting, an incoming e-mail from Twitter popped up on my screen.

We’ve missed you on Twitter!

So much is happening right now on Twitter, and building a great timeline is the way to really enjoy the service. Get to Twitter and start building a timeline that reflects you and your interests, you’ll see how quickly Twitter becomes an invaluable part of your life.

I don’t think so…

Update: At his blog, Matt explains that he wasn’t accusing me of anything. It was CMS and ATLAS physicists who, by telling me me about the results after unblinding, were guilty of ruining the blinded analyses for still top-secret reasons.

Back from vacation today, so regular blogging likely to resume. Will start with something quick, a link to material that was posted today.

The Edge web-site annual question feature is out today, with this year’s question What *Should* We Be Worried About?. I wrote something about the “Nightmare Scenario” that HEP is facing if the LHC finds a Standard Model Higgs and nothing else.

Others addressed the same issue, with Lisa Randall writing:

In my specific field of particle physics, everyone is worried. I don’t say that lightly. I’ve been to two conferences within the last week where the future was a major topic of discussion and I’m at another one where it’s on the agenda.

Her specific concern is motivated by her interest in large extra-dimensional theories, for which no evidence has shown up so far at the LHC. If the extra jump by a factor of 6.5/4 in energy that will arrive in 2015 after repairs still shows nothing, this may be the end of the line for such theories for a very long time. The prospects for a higher energy machine are problematic in terms of technology, as well as the political will to pay for them. The overselling of this that went on for many years pre-LHC won’t make it any easier to re-use these theories as an argument for building a new machine.

Amanda Gefter sees no reason to worry. Particle theorists will just move to making progress without experiment, through studying paradoxes of the current theory, with her final example for optimism the recent debate over the “firewall paradox”.

Carlo Rovelli’s contribution explains one problem with this: humans are very good at convincing themselves they have found some wonderful explanation of something (e.g. some resolution of a paradox, like the supposed SUSY solution to the hierarchy problem), when reality actually involves something quite a bit more subtle and unexpected:

A number of my colleagues in theoretical physics have spent their life studying a possible symmetry of nature called “supersymmetry”. Experiments in laboratories like Geneva’s CERN seem now to be pointing more towards the absence than the presence of this symmetry. I have seen lost stares in the eyes of some colleagues: “Could it be?”, how dare Nature not confirm to our imagination?

By the way, when I was in Paris last week I picked up a copy of Rovelli’s wonderful short book that has just come out in France Et si le temps n’existait pas?. It begins with a personal history of how he got into science, from a background in the 1970s disillusion following the flowering of radical ideas in the 1960, a story I found quite interesting, since I’m of the same generation as him. There’s also the story of how some of the ideas of loop quantum gravity developed, and some speculative material about time. Definitely worth looking for if you read French and are interested in these topics.

Back when I was a student I remember learning that there were two possible sign conventions to use for the Minkowski space metric: the “East coast” one, mostly + signs, favored by relativists and Steven Weinberg, and the “West coast” one, mostly – signs, which was the one in Bjorken and Drell. Then, as now, the big centers of influence in US particle theory were on the coasts: Princeton and Harvard on the East coast, Berkeley, Stanford and Caltech on the West (these days one might want to add the KITP at Santa Barbara). I was educated by the Eastern establishment (who sometimes used the “West coast” sign convention), where gauge theory and the new standard model were the order of the day. The West coast, with its remaining pockets of S-matrix theorists and authors of popular books like “The Tao of Physics” and “The Dancing Wu Li Masters”, was considered to be rather behind the times and a bit soft in the head, perhaps attributable to too much time spent in hot tubs at Esalen and too much use of the agricultural products of Mendocino and Humboldt county.

Remarkably, these days the two coasts remain dominant, with US Fundamental Physics Prizes going only to theorists living within a relatively short drive to an ocean beach. An East coast – West coast disjunction in interests remains, one that it remains tempting to speculate may have something to do with California’s main cash crop. For quite a few years the West coast has been the center of multiverse-mania, and I’ve often wondered what the theorists there would turn to when that lost its “new cutting-edge theory” shine.

It remains unclear what will happen in the long-term, but there’s now a new hot topic in California these past few months. It was the subject a few weeks ago of a workshop (AKA “brain-storming session”) with 50 or so in attendance at Stanford, and is being described by Raphael Bousso (across the Bay at Berkeley) as “this is probably the most exciting thing that’s happened to me since I entered physics.” A full-blown conference is rumoured for April.

LA-based science writer Jennifer Ouellette does a characteristically excellent job of covering the story, starting here by explaining the appeal of the subject (as well as the problem with explaining it):

To include every last detail, the piece would have had to be a good 6000 words long, and frankly, very few general readers would care to slog through all the gory details. So why even bother to try, if one can’t be comprehensive? Because FIREWALLS! That’s why! Seriously, how cool is this concept? There’s nothing more crowd-pleasing than death by black hole (just ask Neil de Grasse Tyson) and now there could be more than one way to die. Spaghetiffication, or incineration? Take your pick.

Another version of that post, which includes an excellent set of references is here. For her full treatment, see the version at Simons Science News.

All of this started with “AMPS” a July paper by four Santa Barbara physicists that already has 25 citations and counting (although of the three papers on the topic by Susskind, one is already “Withdrawn because the author no longer thinks it is correct”). For more on the topic, you can try Bousso’s Strings 2012 talk, blog entries by Polchinski at Cosmic Variance, Caltech’s John Preskill at Quantum Frontiers, Santa Barbara’s Aron Wall at his Physics and Theology blog, or Robert Helling here. I haven’t myself tried reading these papers, partly because I strongly suspect that I’d end up with the same reaction as Robert:

Now, of course I had to read (some of) the papers and I have to say that I am confused. I admit, I did not get the point. Even more, I cannot understand a large part of the discussion. There is a lot of prose and very little formulas and I have failed to translate the prose to formulas or hard facts for myself. Many of the statements taken at face value do not make sense to me but on the other hand, I know the authors to be extremely clever people and thus the problem is most likely on my end.

The problem may be that Robert isn’t in California, but, like me, is too far East. Someone else brought up in the East coast tradition (and now so far East he has kind of fallen off the edge…) is Lubos Motl, whose reaction to this topic is that the whole thing is Peter Woit’s fault:

AMPS isn’t as bad or as obviously wrong as “gravity as an entropic force” but it’s still wrong and what’s worse about it is that it is pushed by some of the names that are more famous than Erik Verlinde’s name. None of those bad apples would really destroy an otherwise healthy research community but the main problem I see is that the bad apples can no longer be efficiently wrestled with. Or it’s not happening. It doesn’t look like anyone cares at all. Instead, it seems to me that people are defending their subjective and increasingly non-quantitative (and often downright wrong) ideas and these people’s connectedness to the journalists and other folks outside the research community itself and the related populism – instead of the scientific evaluation by those who actually understand the things as experts – have become the key determinants of success.

Will firewall-fever spread from the West coast, or is it just a flash in the pan? Time will tell…

On a personal note, blogging may be lighter than usual for the next couple weeks or so, as I travel further East for a vacation in Spain, Portugal and Paris.

Update: Bee’s comment reminds me that I had planned to include a link to George Musser’s SciAm piece about this.

• This week there’s a conference in Oxford I’d have loved to have been at. Slides from some of the talks are already posted here. The conference is in honor of Graeme Segal’s 70th birthday. Happy Birthday Graeme!
• Physics Today has a very interesting piece about the current state of HEP posted today by Burton Richter, focused on the topic of Should the US join CERN?. On the ILC, with Japan the prospective location, he takes the point of view that it’s most likely to be interesting as a Higgs factory, so a 250 GeV machine will suffice:
  

  The ongoing International Linear Collider (ILC) program is aimed at building and running a 500-GeV machine by 2020. A new ILC design study is scheduled for release in a few months, but by 2020 the LHC should have delivered enough cumulative output to make anything the ILC can produce irrelevant beyond what its lower-energy Higgs-factory option can do.

  Besides this, at the energy frontier the LHC is the only game in town, with HL-LHC and HE-LHC challenging and expensive projects that will dominate the future of the subject. If the US wants to participate, Richter argues that a new, closer formal relationship is needed. The politics here is likely to be tricky, with the US Congress not exactly keen on spending money outside the US, through an organization where the US has little influence.

  About the future he’s most worried about the too high cost of getting to higher energy permanently delivering us into the hands of multiverse mania:

  If our only theory of everything comes down to the landscape model, where we are only one of a zillion universes with the parameters we see as only a statistical accident necessary for life, the game is over. I hope not.

• One of the landscapeologists whose influence Richter is worried about is Joe Polchinski at Santa Barbara. Courtesy of the Milner prize competition, Polchinski is in line for about $3 million more influence if he beats out his two competitors next March, and UCSB has a press release about this. The press release explains that Polchinski is being rewarded for his discovery of “one of the basic building blocks of space time”
  

  According to the award citation, the Physics Frontier Prize recognizes Polchinski’s broad contributions to fundamental physics, most notably the discovery of D-branes. These have been shown to provide the atomic structure of black holes, predicted long ago by Stephen Hawking, and, as such, are one of the basic building blocks of spacetime.

  One goal of the Milner prize is to raise the profile of work that is not Nobel-worthy because it isn’t testable science, by creating a bigger prize for it than the Nobel. Unfortunately I think one side-effect of this is to blur the distinction between things we have evidence for and those that are pure speculation (with “D-branes=basic building block of spacetime” the latter, being promoted to the public as if it were the former).

• Steven Weinberg’s graduate level text on QM, Lectures on Quantum Mechanics, is now out, and I’m very much looking forward to getting a copy soon.
• The Higgs boson is Time Magazine’s Particle of the Year, Fabiola Gianotti runner up for Person of the Year.
• I recently read Benoit Mandelbrot’s posthumously published autobiography The Fractalist: Memoir of a Scientific Maverick, but don’t really have the time or interest to write a review here. Mandelbrot has an unusual life-story, starting with being hidden in war-time France to escape the Nazis.

  The thing that struck me most about the book though was that I had always assumed he was an academic outsider, but the true story is quite different. His family was academic mathematics royalty, with uncle Szolem Mandelbrojt a highly influential French mathematician at the College de France guiding him closely. A big theme of the book is Mandelbrot’s detailed explanation of the debates involved at each stage of his life over what would be his best next career move. There’s more about this than about the mathematics.

  Another reason not to write a review is that I can point to two interesting ones already out there. The Wall Street Journal got Stephen Wolfram to write one, see here, and American Scientist has one by Brian Hayes here. Hayes isn’t exactly kind to Mandelbrot, emphasizing his egotism and desire for recognition:

  Mandelbrot begins one chapter of his memoir with the declaration: “A blessing throughout life: I never wonder who I am.” He is untroubled by doubts or regrets, and untainted by false humility. In these pages you will find no self-effacing disclaimers about standing on the shoulders of giants; if Mandelbrot has seen a little farther, it is because he’s taller. From an early age his scientific hero was Johannes Kepler, and his goal in life was to accomplish something worthy of a modern Kepler, overthrowing an outworn orthodoxy. By his own account, he succeeded brilliantly, with quite a number of “Kepler moments.” (As far as I know, Kepler himself had only one.)

• For another, mathematically more interesting, discussion of a recently departed mathematician with an amazing career, see the AMS Notices article on I. M. Gelfand. Gelfand’s career and influence is a huge topic, so this is just Part I.
• A significant new advance in representation theory is explained nicely by its authors here in terms of the general philosophy of representation theory laid out by Gelfand. A standard topic in representation theory courses is to classify the unitary representations of compact semi-simple Lie groups (highest weight theory), but the question of what happens in the non-compact case is much, much more difficult and still open, with one problem that the representations are infinite-dimensional. This latest paper reports “a finite algorithm for computing the set of irreducible unitary representations of a real reductive group G” with the authors describing their result as follows”
  

  The third step in Gelfand’s program is to describe all of the irreducible
  unitary representations of G. This is the problem of “finding the unitary dual”

  G^{^}_u =_def {equiv. classes of irr. unitary representations of G}

  It is this problem for which we offer a solution (for real reductive G) in this paper. It is far from a completely satisfactory solution for Gelfand’s program; for of course what Gelfand’s program asks is that one should be able to answer interesting questions about all irreducible unitary representations. (Then these answers can be assembled into answers to the questions about the reducible representation π, and finally translated into answers to the original questions about the topological space X on which G acts.) We offer not a list of unitary representations but a method to calculate the list. To answer general questions about unitary representations in this way, one would need to study how the questions interact with our algorithm.

  All of which is to say that we may continue to write papers after this one.

  This sort of representation theory is ferociously technical, with many papers in the subject appearing to have been written only to be read by the very small number of people expert in all these technicalities. This document is surprisingly different, starting off with an accessible introduction to the subject, and then devoting a lot of space to a careful, readable exposition of the details of the necessary technicalities. The subject is still ferociously complex and technical, but this paper gives one a fighting chance to actually understand what is going on if one has the time and energy to read one’s way through it. An admirable and unusual choice of how to write a modern math paper.

Update: A commenter points out a nice article that just appeared in Scientific American, Strange and Stringy, by Subir Sachdev, who explains some recent ideas about using dualities to understand certain condensed matter phenomena.

Classes are over for the semester, and I’ve put together the lecture notes for my undergraduate “Quantum Mechanics for Mathematicians” course, which are available here.

The idea for the course was to try and explain the basics of quantum mechanics, from the point of view of unitary representations of Lie groups. While this is a rather advanced topic, I made an effort to do things quite concretely and start at the most basic level (the only prerequisite for the course was calculus and linear algebra). I hope the notes will be useful both to mathematicians trying to learn something about quantum mechanics as well as to physicists who would like to better understand the mathematics behind the way symmetry principles get used in the subject.

More to come next semester. The initial plan is to start with the fermionic oscillator, move on to path integrals, then relativity, the Dirac equation, and U(1) gauge theory (E and M), ending up with some very basic quantum field theory (non-interacting fields). We’ll see how that turns out and at what point I run out of energy and stop writing.

Any corrections, comments or suggestions about how to improve these notes are most welcome.

Update: Thanks to all for comments, I’m quite pleased to see how many people have been looking at these notes (6600 downloads and counting!). They’ve also made an appearance in surprising places, including here.

For the latest SUSY enthusiast take on the implications of what the LHC has been (not) seeing, your best bet might be yesterday’s talk at the KITP by Nima Arkani-Hamed on Naturalness. An hour and 40 minutes, no slides, nothing much on the blackboard, just him talking about how he now sees things. Some high points:

• If the Higgs turns out to have spin two, he’ll quit physics.
• If the Higgs turns out to be a techni-dilaton, he’ll kill himself.
• At this point, a natural theory would have to be rather baroque, so he favors abandoning naturalness in favor of simplicity.
• The simplest thing is the Standard Model, but that requires too much fine-tuning. He won’t completely abandon naturalness: one part in a million fine-tuning is fine, but the SM fine-tuning problem isn’t. This is the point where he loses me (going from the SM to the vastly more complicated SUSY theories with the needed SUSY breaking seems to me not close to being worth the supposed improvement in the fine-tuning).
• He complains that “Some BSM theorists are giving our field a bad name” by repeatedly making SUSY predictions that turn out to be wrong and changing their story.
• He’s not one of those: he still favors split SUSY, and has since 2004.
• Split SUSY makes a falsifiable prediction: no Higgs gamma-gamma excess. This is of course the same prediction as the Standard Model.
• In his favored version of split SUSY, all SUSY partners are much too heavy to ever be observable except the wino, bino and gluino. He had a lot to say about what observing these would tell us, but not much about what the implications are of not seeing them in the LHC 8 TeV run. Would this just mean “surely they’ll show up at 13 TeV”? Is seeing nothing at 8 TeV consistent with split SUSY? What about seeing nothing at 13 TeV?

In any case, giving up on SUSY is definitely not on the agenda as far as he’s concerned.