# Convolution inverse

I'm currently reading some stuff on Hopf algebras, specifically Hopf Algebras: An Introduction by Sorin Dascalescu, Constantin Nastasescu and Serban Raianu. One proof involves showing that for a Hopf algebra $H$ with antipode $S$ that $$\Delta(S(h)) = \sum S(h^{(2)})\otimes S(h^{(1)})$$ In part of the proof a map $G : H\to H\otimes H$ is defined to be $(S\otimes S)\circ \Delta^{op}$ and the goal is to show that $\Delta$ is a right convolution inverse of $G$. That is that $G\star \Delta = (\eta_{H}\otimes \eta_{H})\circ \varepsilon_H$. The proof given runs as follows: \begin{align*} (G\star \Delta)(h) = \sum G(h^{(1)})\Delta(h^{(2)}) = \sum (S((h^{(1)})^{(2)})\otimes S((h^{(1)})^{(1)})((h^{(2)})^{(1)}\otimes (h^{(2)})^{(2)}) \end{align*} $$=\sum (S(h^{(2)})\otimes S(h^{(1)}))(h^{(3)}\otimes h^{(4)}) = \sum S(h^{(2)})h^{(3)}\otimes S(h^{(1)})h^{(4)}$$ $$= \sum S((h^{(2)})^{(1)})(h^{(2)})^{(2)}\otimes S(h^{(1)})h^{(3)} = \sum \varepsilon(h^{(2)})1\otimes S(h^{(1)})h^{(3)}$$ $$= \sum 1\otimes S(h^{(1)})\varepsilon((h^{(2)})^{(1)})(h^{(2)})^{(2)} = \sum 1\otimes S(h^{(1)})h^{(2)} = 1\otimes \varepsilon(h)1$$ $$= ((\eta_{H}\otimes \eta_{H})\circ \varepsilon_{H})(h)$$ Now, the first line makes sense, but after that seems to turn into magic. I know that Sweedler notation is being heavily used, but it seems they are just magically making the computation work with all the nifty switching of Sweedler indices. Can anyone help clarify what is going on here? Thanks in advance.

-
The third, fifth and seventh equality, those for which there are switches of indices, are nothing but the expression of the coassociativity of $\Delta$ in Sweedler notation. – Adrien Apr 20 '12 at 23:39

As you rightly observed, the poof has much to do with the formalism of the Sweedler notation. I'll try to explain the usuage. Let's start with the identity $$\Delta_2 := (\Delta \otimes id) \circ \Delta =(id \otimes \Delta) \circ \Delta$$ Depending on the position of the outer $\Delta$ one has respective structural identities:
$$\begin{array}{rll} \Delta_2(h) = & \sum h^{(1)} \otimes h^{(2)} \otimes h^{(3)} & \text{(no particular position)} \newline = & \sum (h^{(1)})^{(1)} \otimes (h^{(1)})^{(2)} \otimes h^{(2)} & \text{(1st position)}\newline = & \sum h^{(1)} \otimes (h^{(2)})^{(1)} \otimes (h^{(2)})^{(2)} & \text{(2nd position)} \end{array}$$ I call these "structural identities" since, for example, the same symbol $h^{(1)}$ can have different values in different equations. But it's exactly the philosophy of Sweedler's notation to limit the number of symbols.
Similarly, we have $$\Delta_3 := (id \otimes \Delta \otimes id) \circ \Delta_2= (\Delta \otimes \Delta) \circ \Delta$$ Again, there are structural identities $$\begin{array}{rl} \Delta_3(h) = & \sum h^{(1)} \otimes h^{(2)} \otimes h^{(3)} \otimes h^{(4)}& \newline = & \sum h^{(1)} \otimes (h^{(2)})^{(1)}\otimes (h^{(2)})^{(2)} \otimes h^{(3)} \newline = & \sum (h^{(1)})^{(1)} \otimes (h^{(1)})^{(2)} \otimes (h^{(2)})^{(1)} \otimes (h^{(2)})^{(2)} \newline \end{array}$$ Now let's have a look at the proof in question. Denote the multiplication by $\mu$. The third equality, for example, is obtained by $$\begin{array}{ll} & \sum (S((h^{(1)})^{(2)})\otimes S((h^{(1)})^{(1)})((h^{(2)})^{(1)}\otimes (h^{(2)})^{(2)}) \newline = & \big (\mu \circ ( (S \otimes S)^{op} \otimes id \otimes id)\big )\big (\sum (h^{(1)})^{(2)}\otimes (h^{(1)})^{(1)} \otimes (h^{(2)})^{(1)}\otimes (h^{(2)})^{(2)}\big) \newline = & \big (\mu \circ ( (S \otimes S)^{op} \otimes id \otimes id)\big ) (\sum h^{(1)} \otimes h^{(2)} \otimes h^{(3)} \otimes h^{(4)} ) \newline = & \sum \big(S(h^{(2)}) \otimes S(h^{(1)})\big)\big(h^{(3)} \otimes h^{(4)}\big) \end{array}$$ To obtain the the fith equation, let $$T(h^{(1)} \otimes h^{(2)} \otimes h^{(3)} \otimes h^{(4)}) = h^{(2)} \otimes h^{(3)} \otimes h^{(1)} \otimes h^{(4)}$$ Then: $$\begin{array}{ll} & \sum S(h^{(2)})h^{(3)}\otimes S(h^{(1)})h^{(4)} \newline = & \big( (\mu \circ (S \otimes id) \otimes \mu \circ (S \otimes id)) \circ T\big) \big( \sum h^{(1)} \otimes h^{(2)} \otimes h^{(3)} \otimes h^{(4)} \big) \end{array}$$ Now applying the 2nd structural identity for $\Delta_3$ above yields $$\sum S(h^{(2)})h^{(3)}\otimes S(h^{(1)})h^{(4)} = \sum S((h^{(2)})^{(1)})(h^{(2)})^{(2)}\otimes S(h^{(1)})h^{(3)}$$ Remark: Of course, one usually doesn't make a detour around expressing everything in the form $$\text{homomorphism}(\sum h^{(1)} \otimes h^{(2)} \otimes h^{(3)} \otimes h^{(4)})$$ but directly applies the homomorphisms element-wise. But I hope the principal becomes clearer that way.