Archive for December, 2006

It’s Now Official

Update Tuesday: My sincerest apologies to Sean and friends at Cosmic Variance, who appear to have reinstated my posting rights (for now at least).

Update Sunday: Sigh. Didn’t last long.

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On Cosmic Variance today Sean asks the reader how they might better moderate the comment section on their blog. Of course, banning crackpots would do the trick. And on CV they seem to know exactly who the crackpots are, those CV guys being so much smarter than everybody else. Sean has failed to acknowledge in the post that they have already banned a number of crackpots. And lest there be any doubt that yours truly qualifies, I did the Brutally Honest Personality Test (courtesy of Chad Orzel), so I’m officially a Crackpot (INTJ) personality. On the age-gender balanced score for extroversion I actually managed 0%. You might as well shoot me now.

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M Theory Lesson 6

In the Higgs poll over at PF a whopping 50% of people are voting for no Higgs found in the next three years. Well, back to M Theory again.

Points take many guises. Eventually we will have the option of throwing them away altogether, using topos theory. After all, the question that really needs answering is, what is an observable? But things get pretty interesting before then. In Brannen’s Clifford algebra one hunts out idempotents, which satisfy the simple projector relation tt=t. Similarly, one might use points in projective (twistor) space, described by the Jordan algebra of Michael Rios.

Are there other ways in which points are naturally associated to operators satisfying tt=t? Why yes, using categories in a fairly simple way, as follows. One can think of the objects of a category as the identity arrows on those objects. For example, a set being a discrete category which only has objects, only has identity arrows. Now let t be the target map, sending an arrow f to its target identity arrow tf. Then clearly tt=t. Similarly, one can discuss a source map s.

For those who are really keen on playing, remember that a topology t in the form of an arrow from Omega to Omega in an elementary topos also obeys the relation tt=t.

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Review Reviewed

I’m not the first, but it looks like fun: the String theorist Polchinski has a review in American Scientist about the two books The Trouble with Physics and Not Even Wrong. I agree with much of his critique, so I will focus on reviewing the String aspects of the review.

The Standard Model is a quantum field theory…

OK, we have a problem right here at the start. The Standard Model is just that: a model. But we’ll let this go, since it’s just semantics and such language is common usage.

…in which particles behave as mathematical points…

OK, this one is a bigger problem. What does he mean by point? How are Strings background independent if particles have no meaning independent of classical points? Somehow I don’t think Polchinski is thinking of functors between toposes when he uses the word point.

Smolin presents the rise and fall of string theory as a morality play… But this story, however grippingly told, is more a work of drama than of history.

Yes, this is quite true, but it isn’t really surprising for a String theorist to think so. And why do they all keep going on about this vacuum energy idea?

The review then moves on to background independence. No wonder these guys can’t stop arguing about this. Both sides think their ideas are more background independent than the other. So long as spin foams ignores things like AdS/CFT and T-duality they cannot possibly be talking about gravity, and on the other hand, as mentioned above, particles may be localised but a point is not just some piece of classical moduli. If one is willing to dive head first into Derived Categories it is difficult to understand why this is not understood. Sigh.

New physical theories are often discovered using a mathematical language that is not the most suitable for them.

Hang on a minute! What theory? I don’t see any theory. Some nice maths, sure. But when you talk about T-duality there is never any discussion of Machian principles or experimental evidence for them. If I’ve missed such papers, please direct me to them! Ahh, wait a minute. They call it the Holographic Principle. Nice idea, but we don’t actually get any physics from the way it is formulated. Again, if I’m wrong about this, please tell me!

Extending this principle to spaces with the edges free will require a major new insight.

Er, like a new Machian principle maybe? Would it be a problem if we threw out the Stringy particle zoo?

It is possible that the solution to this problem already exists among the alternative approaches that Smolin favors.

Er, well, no. That’s not to say that it does not exist. Later on, the review sinks back into a discussion on Dark Energy.

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Back to Business

Hello again! Connection problems here are finally sorted out, so we can get back to business. It was too nice a day yesterday to stay inside anyway. I went with some kea friends to the Basin in Ku-ring-gai where we went swimming and visited a local wallaby, who had a little baby joey in her pouch.

It is very easy to grow impatient in a city. Some things just cannot happen unless conditions are exactly right. Take Fyfe Pass, for example. In Fyfe’s day the ice was much thicker than it is now. These days it isn’t exactly what one would call a pass, but one can still cross, given the right conditions: a fine day in late spring after the cirque has avalanched out and left a high pile of debris almost to the top of the bluff at the base of the gut. It’s simple climbing from there really, with only one flaky abseil across the waterfall. A lot of things are like that. Not so hard when you look at them the right way.

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Bloggy Bloom

Having installed a CQ Counter a week or two ago, I have been able to watch what sort of people visit this site. Very entertaining. I have also been getting emails from complete strangers about comments on my blog. Isn’t it nice to know that someone is paying attention? In mountaineering there is a term for getting someone to follow you casually, secure in their knowledge that they know more than you do: it’s called sandbagging.

Other physics blogs have been rather quiet lately, with the exception of Babe in the Universe and Clifford, who likes to chat. Clifford says he’s going to remember one of my nutty lines for his next Hollywood party. He’s so sweet. People must be busy working productively, as they put it. Well, I guess I should get back to the abstract nonsense then.

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Back to the Future

Well, I feel that one’s Morgan-Phoa blogging duties must not be neglected. It was a wonderful week at ANU, thanks to the hospitality of Amnon Neeman, James Borger and Boris Chorny. It was very hot and dry, except for one cool evening, which we spent feasting at Tosolini’s. Most of us stayed at Toad Hall, which is a whole 150m from the Maths building!

The format was informal, the idea being to speak about some big problem in one’s own area of interest that should have wider appeal. I have never been to a workshop where this worked so well. Tuesday kicked off with Steve Lack giving an introductory talk on Topos Theory. For this week the term introductory assumes that one is either really into Category Theory or really, really good at Algebraic Geometry or Homotopy Theory.

James Borger followed with some revision on Algebraic Spaces and a question about related, weaker topos like structure. To begin with, an old problem with Rng, the category of rings, is that it doesn’t have nice limits for doing Algebraic Geometry. The traditional solution is to use schemes. But then one ends up relying on the Axiom of Choice even though it isn’t really needed, and the whole theory is very complicated. So instead of a category of schemes one defines a category AlgSp of Algebraic Spaces. This is the opposite category to Rng (= affine schemes) equipped with an etale topology. So things start to look more topos theoretic. James wants to think of a subfunctor from AlgSp into etale sheaves as a kind of half topos.

Boris Chorny modestly launched into some pretty technical ideas on small presheaves. A motivation for his questions was the Motivic Homotopy of Voevodsky, something I would dearly like to understand if I lived another 100 years. This means looking at functors from (wait for it) the opposite category of finite smooth schemes over S with the Nisnevich topology into the category of simplicial sets. Boris says that the new understanding of Motivic Spaces means that we need to redo the classical theory. For instance, is there a way of doing Motivic Homotopy in bigger categories?

Mark Weber spoke about 2-toposes. He has been doing some very interesting work on this. A nice example should be a category of categories CAT. So what is the analogue of the subobject classifier and truth arrow? One thing that works is the forgetful functor from pointed sets into Set. So the suboject classifier becomes the whole category Set! Mark’s notion of 2-topos has the advantage of being able to axiomatise the notion of size. Other examples are based on internal categories in globular sets.

On Tuesday afternoon we had a departmental seminar by Ross Street on his recent work (with Craig Pastro) on quantum categories and weak Hopf algebras in braided monoidal categories. I will talk about this at some later date.

Wednesday morning was Operad Time. Yummy! After a short talk by a certain disreputable physicist, Michael Batanin asked the participants about homotopy types and the search for an ideal theorem about their characterisation by higher groupoids. Fortunately this involved some introductory words on higher operads. Things get particularly interesting when one gets to dimension three. 3-homotopy types require Gray groupoids. These arise as algebras of the Gray 3-operad G. Let’s briefly describe this. For the 0-tree and for any 1-tree, G is the singleton. For a 2-tree which is labelled by ordinals (m1,m2,…,mk), G is the shuffles on (m1,m2,…,mk). And finally, for a 3-tree G is given by a Cartesian product of G for the boundary 2-trees. This structure is due to the weakened interchange law of Gray categories. The question is: what are the higher dimensional analogues of this operad? Batanin also gave the Colloquium talk on Thurdsday afternoon, about the relation of his work to Deligne’s conjecture.

Simona Paoli was wondering about a model structure for internal categories. She discussed a 2005 paper by Everaert et al and open questions related to the Tamsamani approach to higher categories. This involves some intriguing looking cubical structures, which I don’t understand at all. Alexei Davydov then spoke about autoequivalences, and Amnon Neeman about equivalences for derived categories.

On Thursday morning we were visited by Peter Bouwknegt, who posed the question of a good definition for C* algebra objects in monoidal categories, with motivation from his work on T-duality. At this point there was some laughter on the invasion of physics into such a pure mathematics workshop. Later on we actually found some time for more introductory talks. Boris Chorny told us about the Calculus of Functors. He focused on a dictionary between the traditional calculus of functions and the Homotopy Calculus. To begin with, instead of a function from a manifold M into R one has a functor from pointed topological spaces into either a category of topological spaces or a category of spectra. The notion of |x – y| small becomes f: X –> Y is highly connected. The replacement of derivatives defined using h–>0 is quite abstract: the derivative of a functor F with respect to a pointed space X is the homotopy colimit (as n –> oo) of the n-fold loop space of the homotopy fibrations of F(X v S^n) –> F(X). Er, yeah, OK. Anyway, the point is that spheres S^n for large n are like highly contractible spaces. So we had a real h–>0 and now we have a discrete n –> oo.

My favourite talk for the week was the last: James Borger speaking about Lambda Rings and related goodies. But enough blathering from me on all this!

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