The Unapologetic Mathematician

Mathematics for the interested outsider

The Temperley-Lieb Category

Okay, after last week’s shake-ups I’m ready to get back into the swing of things. I mentioned yesterday something called the “Temperley-Lieb Category”, and it just so happens we’re right on schedule to explain it properly.

We’ve seen the category of braids and how the braided coherence theorem makes it the “free braided monoidal category on one object”. That is, it has exactly the structure needed for a braided monoidal category — no more, no less — and if we pick any object in another such category \mathcal{C} we get a unique functor from \mathcal{B}raid to \mathcal{C}.

So of course we want the same sort of thing for monoidal categories with duals. We’ll even draw the same sorts of pictures. A point on a horizontal line will be our generating object, but we also need a dual object. So specifically we’ll think of the object as being “going up through the point” and the dual as “going down through the point”. Then we can draw cups and caps to connect an upward line and a downward line and interpret it as a duality map. Notice, though, that we can’t make any curves cross each other because we have no braiding! Here’s an example of such a Temperley-Lieb diagram:
Oriented Temperley-Lieb diagram

Again, we read this from bottom to top, and from left to right. On the bottom line we have a downward line followed by an upward line, which means we start at the object X^*\otimes X. Then we pass through a cap, which corresponds to the transformation \epsilon_{X^*}. Then we go through a cup (\eta_X^*) to get to X\otimes X^*, and another cup to get to X\otimes X^*\otimes X\otimes X^*. A cap in the middle (\epsilon_{X^*}) is followed by a cup (\eta_X), and then another pair of caps (\epsilon_X\otimes\epsilon_X). Then we have a cup \eta_{X^*} and another \eta_X to end up at X\otimes X^*\otimes X\otimes X^*.

We could simplify this a bit by cancelling two cup/cap pairs using the equations we imposed on the natural transformations \eta and \epsilon. In fact, this is probably a much easier way to remember what those equations mean. The equations tell us in algebraic terms that we can cancel off a neighboring cup and cap, while the topology of diagram says that we can straighten out a zig-zag.

Incidentally, one feature that’s missing from this diagram is that it’s entirely possible to have an arc (pointing either way) start at the bottom of the diagram and leave at the top.

Now if we have any category \mathcal{C} with duals and an object C we can build a unique functor from the category \mathcal{OTL} of oriented Temperley-Lieb diagrams to \mathcal{C} sending the upwards-oriented line to the object C. It sends the above diagram (for example) to the morphism

\left[(1_C\otimes\eta_C\otimes1_{C^*})\circ\eta_{C^*}\circ(\epsilon_C\otimes\epsilon_C)\circ(1_C\otimes\eta_C\otimes1_{C^*})\circ(1_C\otimes\epsilon_{C^*}\otimes1_{C^*})\circ(1_C\otimes1_C^*\otimes\eta_{C^*})\circ\eta_{C^*}\circ\epsilon_{C^*}\right]:
C^*\otimes C\rightarrow C\otimes C^*\otimes C\otimes C^*.

Another useful category is the free monoidal category with duals on a single self-dual object. This is the Temperley-Lieb category \mathcal{TL} which looks just the same as \mathcal{OTL} with one crucial difference: since the object X is its own dual, we can’t tell the difference between the two different directions a line could go. Up and down are the same thing. In the algebra this might seem a little odd, but in the diagram all it means is we get to drop the little arrows that tell us which way to go.

And now if we have any category \mathcal{C} with duals and any self-dual object C=C^* we have a unique functor from \mathcal{TL} to \mathcal{C} sending the strand to \mathcal{C}. This is how Temperley-Lieb diagrams are turned into (categorified) \mathfrak{sl}_2 representations in Khovanov homology.

July 12, 2007 Posted by | Category theory, Knot theory | 7 Comments

   

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