Arcadian Functor

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Marni D. Sheppeard

Saturday, February 03, 2007

M Theory Lesson 13

John Baez's TWF244 is really cool. He talks about a recent paper by Leinster on the Euler characteristic of a finite category. Consider the following. Order the objects in the category 1,2,3,,n. The integral adjacency matrix for the category sets aij to be the number of arrows from i to j.

For example, in the category

we would have a 3x3 matrix with all entries 1, since we must not forget the identity arrows. If the inverse to this matrix A existed, the Euler characteristic would be the sum of entries in A-1. Let's fill in a few more arrows. Imagine there were k arrows from 1 to 2, 2 to 3 and 1 to 3 which forms a basic composition triangle. Similarly, imagine the dual triangle had m arrows at each edge. Then the adjacency matrix would be a circulant based on 1,k and m. Such triangles look like idempotent equations k2=k, but here k is an ordinal and we should wonder about composing one of the k arrows from 1 to 2 with another one from 2 to 3, because the number of such compositions would naively be more than k. If k2=k were true, and k was ordinal, then it must be zero or one, which gives a particularly simple kind of category otherwise known as a poset.

Anyway, to cut a long story short, this characteristic works nicely for all sorts of things, such as orbifolds. In M Theory we counted the number of particle generations using an orbifold Euler characteristic, which might be a rational number in general. So we can think of this as a cardinality of a category! This is wonderful, because the physical result follows from the universality of χ.

Moerdijk looked at Lie groupoids as a foundation for orbifolds, which seems like a logical thing to do from the Symmetry point of view. But remember that we encountered the orbifold Euler characteristic in the work of Mulase et al on ribbon matrix models.

6 Comments:

Blogger L. Riofrio said...

These diagrams look similiar to the Eightfold Way. That makes one wonder whether non-linear operads will be key to extending the Standard Model. That would be refreshing, since physics has gone nowhere in 30 years.

February 04, 2007 10:08 AM  
Blogger Kea said...

Yeah. And the ribbon diagrams are just what 't Hooft ordered for QCD back in 1974. Seems so simple, doesn't it?

February 04, 2007 12:36 PM  
Anonymous Anonymous said...

Hi Kea

Thanks for the link to TWF 244. As usual John Baez has a great and interesting blog.

I am fascinated with item 5 which discusses Euler’s bridges. From my perspective this is a problem ideal for the strategy analysis of game theory.

Geert Jan Olsder [mathematics] Delft University in 2005 presented a variant of this problem as a train routing schedule using game theory.
MAX PLUS IN HET (TREIN)VERKEER ...[Text in English]
webserv.nhl.nl/~kamminga/wintersymposium/Olsder2005.pdf

If you like, on Amazon.com you can view inside this great book: Dynamic Noncooperative Game Theory (Classics in Applied Mathematics) (Paperback)
by Tamer Basar, Geert Jan Olsder.

Basar is also still active as a Professor of Electrical and Computer Engineering. Engineers might be considered “applied physicists“.

February 04, 2007 1:49 PM  
Blogger Kea said...

Doug, we appreciate your enthusiasm for Game Theory, but I have to say, I'm not sure when I'm going to find time to read any of these references, once I slog through a few papers in particle physics, math phys, maths, cosmology, philosophy ..... sigh. So little time.

February 04, 2007 2:09 PM  
Anonymous Anonymous said...

Thanks for the Leinster reference Kea. I'm pleased to know that whatever the fundamental objects of M-theory are, we can still talk about their Euler characteristic!

February 04, 2007 7:35 PM  
Blogger Kea said...

Why, yes, kneemo! This is important. We can't go to all this trouble to create a 'true BI' theory and then throw it all out by cheating on the actual number crunching at the end. The numbers must fall out of a universal construction.

February 05, 2007 10:05 AM  

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