pnas/pnas.tex
changeset 580 99611dfed1f3
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   379 if there exists a permissible decomposition $M_0\to\cdots\to M_m = W$ such that
   379 if there exists a permissible decomposition $M_0\to\cdots\to M_m = W$ such that
   380 each $B_i$ appears as a connected component of one of the $M_j$. Note that this allows the balls to be pairwise either disjoint or nested. Such a collection of balls cuts $W$ into pieces, the connected components of $W \setminus \bigcup \bdy B_i$. These pieces need not be manifolds, but they do automatically have permissible decompositions.
   380 each $B_i$ appears as a connected component of one of the $M_j$. Note that this allows the balls to be pairwise either disjoint or nested. Such a collection of balls cuts $W$ into pieces, the connected components of $W \setminus \bigcup \bdy B_i$. These pieces need not be manifolds, but they do automatically have permissible decompositions.
   381 
   381 
   382 The $k$-blob group $\bc_k(W; \cC)$ is generated by the $k$-blob diagrams. A $k$-blob diagram consists of
   382 The $k$-blob group $\bc_k(W; \cC)$ is generated by the $k$-blob diagrams. A $k$-blob diagram consists of
   383 \begin{itemize}
   383 \begin{itemize}
   384 \item a permissible collection of $k$ embedded balls (called `blobs') in $W$,
   384 \item a permissible collection of $k$ embedded balls,
   385 \item an ordering of the balls, and
   385 \item an ordering of the balls, and
   386 \item for each resulting piece of $W$, a field,
   386 \item for each resulting piece of $W$, a field,
   387 \end{itemize}
   387 \end{itemize}
   388 such that for any innermost blob $B$, the field on $B$ goes to zero under the composition map from $\cC$.
   388 such that for any innermost blob $B$, the field on $B$ goes to zero under the composition map from $\cC$. We call such a field a `null field on $B$'.
   389 
   389 
   390 The differential acts on a $k$-blob diagram by summing over ways to forget one of the $k$ blobs, with signs given by the ordering.
   390 The differential acts on a $k$-blob diagram by summing over ways to forget one of the $k$ blobs, with signs given by the ordering.
   391 
   391 
   392 \todo{Say why this really is the homotopy colimit}
   392 \todo{Say why this really is the homotopy colimit}
   393 \todo{Spell out $k=0, 1, 2$}
   393 
       
   394 We now spell this out for some small values of $k$. For $k=0$, the $0$-blob group is simply fields on $W$. For $k=1$, a generator consists of a field on $W$ and a ball, such that the restriction of the field that that ball is a null field. The differential simply forgets the ball. Thus we see that $H_0$ of the blob complex is the quotient of fields by null fields.
       
   395 
       
   396 For $k=2$, we have a two types of generators; they each consists of a field $f$ on $W$, and two balls $B_1$ and $B_2$. In the first case, the balls are disjoint, and $f$ restricted to either of the $B_i$ is a null field. In the second case, the balls are properly nested, say $B_1 \subset B_2$, and $f$ restricted to $B_1$ is null. Note that this implies that $f$ restricted to $B_2$ is also null, by the associativity of the gluing operation. This ensures that the differential is well-defined.
   394 
   397 
   395 \section{Properties of the blob complex}
   398 \section{Properties of the blob complex}
   396 \subsection{Formal properties}
   399 \subsection{Formal properties}
   397 \label{sec:properties}
   400 \label{sec:properties}
   398 The blob complex enjoys the following list of formal properties.
   401 The blob complex enjoys the following list of formal properties.
   588 $$\bc_*(X; \pi^\infty_{\le n}(T)) \simeq \CM{X}{T}.$$
   591 $$\bc_*(X; \pi^\infty_{\le n}(T)) \simeq \CM{X}{T}.$$
   589 \end{thm}
   592 \end{thm}
   590 
   593 
   591 This says that we can recover (up to homotopy) the space of maps to $T$ via blob homology from local data. 
   594 This says that we can recover (up to homotopy) the space of maps to $T$ via blob homology from local data. 
   592 Note that there is no restriction on the connectivity of $T$ as there is for the corresponding result in topological chiral homology \cite[Theorem 3.8.6]{0911.0018}.
   595 Note that there is no restriction on the connectivity of $T$ as there is for the corresponding result in topological chiral homology \cite[Theorem 3.8.6]{0911.0018}.
   593 
   596 \todo{sketch proof}
   594 
   597 
   595 \begin{thm}[Higher dimensional Deligne conjecture]
   598 \begin{thm}[Higher dimensional Deligne conjecture]
   596 \label{thm:deligne}
   599 \label{thm:deligne}
   597 The singular chains of the $n$-dimensional surgery cylinder operad act on blob cochains.
   600 The singular chains of the $n$-dimensional surgery cylinder operad act on blob cochains.
   598 Since the little $n{+}1$-balls operad is a suboperad of the $n$-SC operad,
   601 Since the little $n{+}1$-balls operad is a suboperad of the $n$-SC operad,
   599 this implies that the little $n{+}1$-balls operad acts on blob cochains of the $n$-ball.
   602 this implies that the little $n{+}1$-balls operad acts on blob cochains of the $n$-ball.
   600 \end{thm}
   603 \end{thm}
   601 
   604 
   602 An $n$-dimensional surgery cylinder is an alternating sequence of mapping cylinders and surgeries, modulo changing the order of distant surgeries, and conjugating a submanifold not modified in a surgery by a homeomorphism. See Figure \ref{delfig2}. Surgery cylinders form an operad, by gluing the outer boundary of one cylinder into an inner boundary of another.
   605 An $n$-dimensional surgery cylinder is a sequence of mapping cylinders and surgeries (Figure \ref{delfig2}), modulo changing the order of distant surgeries, and conjugating a submanifold not modified in a surgery by a homeomorphism. Surgery cylinders form an operad, by gluing the outer boundary of one cylinder into an inner boundary of another.
   603 
   606 
   604 
   607 By the `blob cochains' of a manifold $X$, we mean the $A_\infty$ maps of $\bc_*(X)$ as a $\bc_*(\bdy X)$ $A_\infty$-module.
   605 
   608 
   606 \todo{Explain blob cochains}
       
   607 \todo{Sketch proof}
   609 \todo{Sketch proof}
   608 
   610 
   609 The little disks operad $LD$ is homotopy equivalent to the $n=1$ case of the $n$-SC operad. The blob complex $\bc_*(I, \cC)$ is a bimodule over itself, and the $A_\infty$-bimodule intertwiners are homotopy equivalent to the Hochschild cohains $Hoch^*(C, C)$. The usual Deligne conjecture (proved variously in \cite{hep-th/9403055, MR1805894, MR2064592, MR1805923} gives a map
   611 The little disks operad $LD$ is homotopy equivalent to the $n=1$ case of the $n$-SC operad. The blob complex $\bc_*(I, \cC)$ is a bimodule over itself, and the $A_\infty$-bimodule intertwiners are homotopy equivalent to the Hochschild cohains $Hoch^*(C, C)$. The usual Deligne conjecture (proved variously in \cite{hep-th/9403055, MR1805894, MR2064592, MR1805923}) gives a map
   610 \[
   612 \[
   611 	C_*(LD_k)\otimes \overbrace{Hoch^*(C, C)\otimes\cdots\otimes Hoch^*(C, C)}^{\text{$k$ copies}}
   613 	C_*(LD_k)\otimes \overbrace{Hoch^*(C, C)\otimes\cdots\otimes Hoch^*(C, C)}^{\text{$k$ copies}}
   612 			\to  Hoch^*(C, C),
   614 			\to  Hoch^*(C, C),
   613 \]
   615 \]
   614 which we now see to be a specialization of Theorem \ref{thm:deligne}.
   616 which we now see to be a specialization of Theorem \ref{thm:deligne}.