diff -r 408abd5ef0c7 -r adc03f9d8422 text/blobdef.tex --- /dev/null Thu Jan 01 00:00:00 1970 +0000 +++ b/text/blobdef.tex Tue Mar 02 20:07:31 2010 +0000 @@ -0,0 +1,189 @@ +%!TEX root = ../blob1.tex + +\section{The blob complex} +\label{sec:blob-definition} + +Let $X$ be an $n$-manifold. +Assume a fixed system of fields and local relations. +In this section we will usually suppress boundary conditions on $X$ from the notation +(e.g. write $\lf(X)$ instead of $\lf(X; c)$). + +We want to replace the quotient +\[ + A(X) \deq \lf(X) / U(X) +\] +of the previous section with a resolution +\[ + \cdots \to \bc_2(X) \to \bc_1(X) \to \bc_0(X) . +\] + +We will define $\bc_0(X)$, $\bc_1(X)$ and $\bc_2(X)$, then give the general case $\bc_k(X)$. + +We of course define $\bc_0(X) = \lf(X)$. +(If $X$ has nonempty boundary, instead define $\bc_0(X; c) = \lf(X; c)$. +We'll omit this sort of detail in the rest of this section.) +In other words, $\bc_0(X)$ is just the space of all linearized fields on $X$. + +$\bc_1(X)$ is, roughly, the space of all local relations that can be imposed on $\bc_0(X)$. +Less roughly (but still not the official definition), $\bc_1(X)$ is finite linear +combinations of 1-blob diagrams, where a 1-blob diagram to consists of +\begin{itemize} +\item An embedded closed ball (``blob") $B \sub X$. +\item A field $r \in \cC(X \setmin B; c)$ +(for some $c \in \cC(\bd B) = \cC(\bd(X \setmin B))$). +\item A local relation field $u \in U(B; c)$ +(same $c$ as previous bullet). +\end{itemize} +(See Figure \ref{blob1diagram}.) +\begin{figure}[!ht]\begin{equation*} +\mathfig{.9}{definition/single-blob} +\end{equation*}\caption{A 1-blob diagram.}\label{blob1diagram}\end{figure} +In order to get the linear structure correct, we (officially) define +\[ + \bc_1(X) \deq \bigoplus_B \bigoplus_c U(B; c) \otimes \lf(X \setmin B; c) . +\] +The first direct sum is indexed by all blobs $B\subset X$, and the second +by all boundary conditions $c \in \cC(\bd B)$. +Note that $\bc_1(X)$ is spanned by 1-blob diagrams $(B, u, r)$. + +Define the boundary map $\bd : \bc_1(X) \to \bc_0(X)$ by +\[ + (B, u, r) \mapsto u\bullet r, +\] +where $u\bullet r$ denotes the linear +combination of fields on $X$ obtained by gluing $u$ to $r$. +In other words $\bd : \bc_1(X) \to \bc_0(X)$ is given by +just erasing the blob from the picture +(but keeping the blob label $u$). + +Note that the skein space $A(X)$ +is naturally isomorphic to $\bc_0(X)/\bd(\bc_1(X))) = H_0(\bc_*(X))$. + +$\bc_2(X)$ is, roughly, the space of all relations (redundancies) among the +local relations encoded in $\bc_1(X)$. +More specifically, $\bc_2(X)$ is the space of all finite linear combinations of +2-blob diagrams, of which there are two types, disjoint and nested. + +A disjoint 2-blob diagram consists of +\begin{itemize} +\item A pair of closed balls (blobs) $B_0, B_1 \sub X$ with disjoint interiors. +\item A field $r \in \cC(X \setmin (B_0 \cup B_1); c_0, c_1)$ +(where $c_i \in \cC(\bd B_i)$). +\item Local relation fields $u_i \in U(B_i; c_i)$, $i=1,2$. \nn{We're inconsistent with the indexes -- are they 0,1 or 1,2? I'd prefer 1,2.} +\end{itemize} +(See Figure \ref{blob2ddiagram}.) +\begin{figure}[!ht]\begin{equation*} +\mathfig{.9}{definition/disjoint-blobs} +\end{equation*}\caption{A disjoint 2-blob diagram.}\label{blob2ddiagram}\end{figure} +We also identify $(B_0, B_1, u_0, u_1, r)$ with $-(B_1, B_0, u_1, u_0, r)$; +reversing the order of the blobs changes the sign. +Define $\bd(B_0, B_1, u_0, u_1, r) = +(B_1, u_1, u_0\bullet r) - (B_0, u_0, u_1\bullet r) \in \bc_1(X)$. +In other words, the boundary of a disjoint 2-blob diagram +is the sum (with alternating signs) +of the two ways of erasing one of the blobs. +It's easy to check that $\bd^2 = 0$. + +A nested 2-blob diagram consists of +\begin{itemize} +\item A pair of nested balls (blobs) $B_0 \sub B_1 \sub X$. +\item A field $r \in \cC(X \setmin B_0; c_0)$ +(for some $c_0 \in \cC(\bd B_0)$), which is splittable along $\bd B_1$. +\item A local relation field $u_0 \in U(B_0; c_0)$. +\end{itemize} +(See Figure \ref{blob2ndiagram}.) +\begin{figure}[!ht]\begin{equation*} +\mathfig{.9}{definition/nested-blobs} +\end{equation*}\caption{A nested 2-blob diagram.}\label{blob2ndiagram}\end{figure} +Let $r = r_1 \bullet r'$, where $r_1 \in \cC(B_1 \setmin B_0; c_0, c_1)$ +(for some $c_1 \in \cC(B_1)$) and +$r' \in \cC(X \setmin B_1; c_1)$. +Define $\bd(B_0, B_1, u_0, r) = (B_1, u_0\bullet r_1, r') - (B_0, u_0, r)$. +Note that the requirement that +local relations are an ideal with respect to gluing guarantees that $u_0\bullet r_1 \in U(B_1)$. +As in the disjoint 2-blob case, the boundary of a nested 2-blob is the alternating +sum of the two ways of erasing one of the blobs. +If we erase the inner blob, the outer blob inherits the label $u_0\bullet r_1$. +It is again easy to check that $\bd^2 = 0$. + +As with the 1-blob diagrams, in order to get the linear structure correct it is better to define +(officially) +\begin{eqnarray*} + \bc_2(X) & \deq & + \left( + \bigoplus_{B_0, B_1 \text{disjoint}} \bigoplus_{c_0, c_1} + U(B_0; c_0) \otimes U(B_1; c_1) \otimes \lf(X\setmin (B_0\cup B_1); c_0, c_1) + \right) \\ + && \bigoplus \left( + \bigoplus_{B_0 \subset B_1} \bigoplus_{c_0} + U(B_0; c_0) \otimes \lf(X\setmin B_0; c_0) + \right) . +\end{eqnarray*} +The final $\lf(X\setmin B_0; c_0)$ above really means fields splittable along $\bd B_1$, +but we didn't feel like introducing a notation for that. +For the disjoint blobs, reversing the ordering of $B_0$ and $B_1$ introduces a minus sign +(rather than a new, linearly independent 2-blob diagram). + +Now for the general case. +A $k$-blob diagram consists of +\begin{itemize} +\item A collection of blobs $B_i \sub X$, $i = 0, \ldots, k-1$. +For each $i$ and $j$, we require that either $B_i$ and $B_j$have disjoint interiors or +$B_i \sub B_j$ or $B_j \sub B_i$. +(The case $B_i = B_j$ is allowed. +If $B_i \sub B_j$ the boundaries of $B_i$ and $B_j$ are allowed to intersect.) +If a blob has no other blobs strictly contained in it, we call it a twig blob. +\item Fields (boundary conditions) $c_i \in \cC(\bd B_i)$. +(These are implied by the data in the next bullets, so we usually +suppress them from the notation.) +$c_i$ and $c_j$ must have identical restrictions to $\bd B_i \cap \bd B_j$ +if the latter space is not empty. +\item A field $r \in \cC(X \setmin B^t; c^t)$, +where $B^t$ is the union of all the twig blobs and $c^t \in \cC(\bd B^t)$ +is determined by the $c_i$'s. +$r$ is required to be splittable along the boundaries of all blobs, twigs or not. +\item For each twig blob $B_j$ a local relation field $u_j \in U(B_j; c_j)$, +where $c_j$ is the restriction of $c^t$ to $\bd B_j$. +If $B_i = B_j$ then $u_i = u_j$. +\end{itemize} +(See Figure \ref{blobkdiagram}.) +\begin{figure}[!ht]\begin{equation*} +\mathfig{.9}{definition/k-blobs} +\end{equation*}\caption{A $k$-blob diagram.}\label{blobkdiagram}\end{figure} + +If two blob diagrams $D_1$ and $D_2$ +differ only by a reordering of the blobs, then we identify +$D_1 = \pm D_2$, where the sign is the sign of the permutation relating $D_1$ and $D_2$. + +$\bc_k(X)$ is, roughly, all finite linear combinations of $k$-blob diagrams. +As before, the official definition is in terms of direct sums +of tensor products: +\[ + \bc_k(X) \deq \bigoplus_{\overline{B}} \bigoplus_{\overline{c}} + \left( \otimes_j U(B_j; c_j)\right) \otimes \lf(X \setmin B^t; c^t) . +\] +Here $\overline{B}$ runs over all configurations of blobs, satisfying the conditions above. +$\overline{c}$ runs over all boundary conditions, again as described above. +$j$ runs over all indices of twig blobs. The final $\lf(X \setmin B^t; c^t)$ must be interpreted as fields which are splittable along all of the blobs in $\overline{B}$. + +The boundary map $\bd : \bc_k(X) \to \bc_{k-1}(X)$ is defined as follows. +Let $b = (\{B_i\}, \{u_j\}, r)$ be a $k$-blob diagram. +Let $E_j(b)$ denote the result of erasing the $j$-th blob. +If $B_j$ is not a twig blob, this involves only decrementing +the indices of blobs $B_{j+1},\ldots,B_{k-1}$. +If $B_j$ is a twig blob, we have to assign new local relation labels +if removing $B_j$ creates new twig blobs. +If $B_l$ becomes a twig after removing $B_j$, then set $u_l = u_j\bullet r_l$, +where $r_l$ is the restriction of $r$ to $B_l \setmin B_j$. +Finally, define +\eq{ + \bd(b) = \sum_{j=0}^{k-1} (-1)^j E_j(b). +} +The $(-1)^j$ factors imply that the terms of $\bd^2(b)$ all cancel. +Thus we have a chain complex. + +\nn{?? say something about the ``shape" of tree? (incl = cone, disj = product)} + +\nn{?? remark about dendroidal sets?; probably not} + +