text/deligne.tex
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%!TEX root = ../blob1.tex
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\section{Higher-dimensional Deligne conjecture}
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\label{sec:deligne}
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In this section we 
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sketch
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\nn{revisit ``sketch" after proof is done} 
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the proof of a higher dimensional version of the Deligne conjecture
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about the action of the little disks operad on Hochschild cohomology.
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The first several paragraphs lead up to a precise statement of the result
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(Proposition \ref{prop:deligne} below).
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Then we sketch the proof.
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\nn{Does this generalisation encompass Kontsevich's proposed generalisation from \cite{MR1718044}, that (I think...) the Hochschild homology of an $E_n$ algebra is an $E_{n+1}$ algebra? -S}
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%from http://www.ams.org/mathscinet-getitem?mr=1805894
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%Different versions of the geometric counterpart of Deligne's conjecture have been proven by Tamarkin [``Formality of chain operad of small squares'', preprint, http://arXiv.org/abs/math.QA/9809164], the reviewer [in Confˇrence Moshˇ Flato 1999, Vol. II (Dijon), 307--331, Kluwer Acad. Publ., Dordrecht, 2000; MR1805923 (2002d:55009)], and J. E. McClure and J. H. Smith [``A solution of Deligne's conjecture'', preprint, http://arXiv.org/abs/math.QA/9910126] (see also a later simplified version [J. E. McClure and J. H. Smith, ``Multivariable cochain operations and little $n$-cubes'', preprint, http://arXiv.org/abs/math.QA/0106024]). The paper under review gives another proof of Deligne's conjecture, which, as the authors indicate, may be generalized to a proof of a higher-dimensional generalization of Deligne's conjecture, suggested in [M. Kontsevich, Lett. Math. Phys. 48 (1999), no. 1, 35--72; MR1718044 (2000j:53119)]. 
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The usual Deligne conjecture (proved variously in \cite{MR1805894, MR2064592, hep-th/9403055, MR1805923} gives a map
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\[
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	C_*(LD_k)\otimes \overbrace{Hoch^*(C, C)\otimes\cdots\otimes Hoch^*(C, C)}^{\text{$k$ copies}}
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			\to  Hoch^*(C, C) .
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\]
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Here $LD_k$ is the $k$-th space of the little disks operad, and $Hoch^*(C, C)$ denotes Hochschild
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cochains.
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The little disks operad is homotopy equivalent to the 
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(transversely orient) fat graph operad
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\nn{need ref, or say more precisely what we mean}, 
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and Hochschild cochains are homotopy equivalent to $A_\infty$ endomorphisms
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of the blob complex of the interval, thought of as a bimodule for itself.
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\nn{need to make sure we prove this above}.
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So the 1-dimensional Deligne conjecture can be restated as
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\[
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	C_*(FG_k)\otimes \hom(\bc^C_*(I), \bc^C_*(I))\otimes\cdots
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	\otimes \hom(\bc^C_*(I), \bc^C_*(I))
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	  \to  \hom(\bc^C_*(I), \bc^C_*(I)) .
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\]
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See Figure \ref{delfig1}.
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\begin{figure}[!ht]
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$$\mathfig{.9}{deligne/intervals}$$
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\caption{A fat graph}\label{delfig1}\end{figure}
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We emphasize that in $\hom(\bc^C_*(I), \bc^C_*(I))$ we are thinking of $\bc^C_*(I)$ as a module
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for the $A_\infty$ 1-category associated to $\bd I$, and $\hom$ means the 
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morphisms of such modules as defined in 
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Subsection \ref{ss:module-morphisms}.
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We can think of a fat graph as encoding a sequence of surgeries, starting at the bottommost interval
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of Figure \ref{delfig1} and ending at the topmost interval.
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The surgeries correspond to the $k$ bigon-shaped ``holes" in the fat graph.
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We remove the bottom interval of the bigon and replace it with the top interval.
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To convert this topological operation to an algebraic one, we need, for each hole, an element of
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$\hom(\bc^C_*(I_{\text{bottom}}), \bc^C_*(I_{\text{top}}))$.
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So for each fixed fat graph we have a map
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\[
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	 \hom(\bc^C_*(I), \bc^C_*(I))\otimes\cdots
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	\otimes \hom(\bc^C_*(I), \bc^C_*(I))  \to  \hom(\bc^C_*(I), \bc^C_*(I)) .
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\]
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If we deform the fat graph, corresponding to a 1-chain in $C_*(FG_k)$, we get a homotopy
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between the maps associated to the endpoints of the 1-chain.
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Similarly, higher-dimensional chains in $C_*(FG_k)$ give rise to higher homotopies.
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It should now be clear how to generalize this to higher dimensions.
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In the sequence-of-surgeries description above, we never used the fact that the manifolds
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involved were 1-dimensional.
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Thus we can define an $n$-dimensional fat graph to be a sequence of general surgeries
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on an $n$-manifold (Figure \ref{delfig2}).
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\begin{figure}[!ht]
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$$\mathfig{.9}{deligne/manifolds}$$
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\caption{An  $n$-dimensional fat graph}\label{delfig2}
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\end{figure}
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More specifically, an $n$-dimensional fat graph ($n$-FG for short) consists of:
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\begin{itemize}
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\item ``Upper" $n$-manifolds $M_0,\ldots,M_k$ and ``lower" $n$-manifolds $N_0,\ldots,N_k$,
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with $\bd M_i = \bd N_i = E_i$ for all $i$.
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We call $M_0$ and $N_0$ the outer boundary and the remaining $M_i$'s and $N_i$'s the inner
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boundaries.
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\item Additional manifolds $R_1,\ldots,R_{k}$, with $\bd R_i = E_0\cup \bd M_i = E_0\cup \bd N_i$.
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%(By convention, $M_i = N_i = \emptyset$ if $i <1$ or $i>k$.)
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\item Homeomorphisms 
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\begin{eqnarray*}
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	f_0: M_0 &\to& R_1\cup M_1 \\
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	f_i: R_i\cup N_i &\to& R_{i+1}\cup M_{i+1}\;\; \mbox{for}\, 1\le i \le k-1 \\
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	f_k: R_k\cup N_k &\to& N_0 .
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\end{eqnarray*}
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Each $f_i$ should be the identity restricted to $E_0$.
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\end{itemize}
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We can think of the above data as encoding the union of the mapping cylinders $C(f_0),\ldots,C(f_k)$,
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with $C(f_i)$ glued to $C(f_{i+1})$ along $R_{i+1}$
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(see Figure xxxx).
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The $n$-manifolds are the ``$n$-dimensional graph" and the $I$ direction of the mapping cylinders is the ``fat" part.
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We regard two such fat graphs as the same if there is a homeomorphism between them which is the 
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identity on the boundary and which preserves the 1-dimensional fibers coming from the mapping
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cylinders.
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More specifically, we impose the following two equivalence relations:
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\begin{itemize}
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\item If $g: R_i\to R'_i$ is a homeomorphism, we can replace
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\begin{eqnarray*}
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	(\ldots, R_{i-1}, R_i, R_{i+1}, \ldots) &\to& (\ldots, R_{i-1}, R'_i, R_{i+1}, \ldots) \\
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	(\ldots, f_{i-1}, f_i, \ldots) &\to& (\ldots, g\circ f_{i-1}, f_i\circ g^{-1}, \ldots),
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\end{eqnarray*}
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leaving the $M_i$ and $N_i$ fixed.
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(Keep in mind the case $R'_i = R_i$.)
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(See Figure xxxx.)
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\item If $M_i = M'_i \du M''_i$ and $N_i = N'_i \du N''_i$ (and there is a
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compatible disjoint union of $\bd M = \bd N$), we can replace
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\begin{eqnarray*}
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	(\ldots, M_{i-1}, M_i, M_{i+1}, \ldots) &\to& (\ldots, M_{i-1}, M'_i, M''_i, M_{i+1}, \ldots) \\
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	(\ldots, N_{i-1}, N_i, N_{i+1}, \ldots) &\to& (\ldots, N_{i-1}, N'_i, N''_i, N_{i+1}, \ldots) \\
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	(\ldots, R_{i-1}, R_i, R_{i+1}, \ldots) &\to& 
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						(\ldots, R_{i-1}, R_i\cup M''_i, R_i\cup N'_i, R_{i+1}, \ldots) \\
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	(\ldots, f_{i-1}, f_i, \ldots) &\to& (\ldots, f_{i-1}, \rm{id}, f_i, \ldots) .
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\end{eqnarray*}
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(See Figure xxxx.)
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\end{itemize}
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Note that the second equivalence increases the number of holes (or arity) by 1.
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We can make a similar identification with the roles of $M'_i$ and $M''_i$ reversed.
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In terms of the ``sequence of surgeries" picture, this says that if two successive surgeries
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do not overlap, we can perform them in reverse order or simultaneously.
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There is an operad structure on $n$-dimensional fat graphs, given by gluing the outer boundary
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of one graph into one of the inner boundaries of another graph.
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We leave it to the reader to work out a more precise statement in terms of $M_i$'s, $f_i$'s etc.
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For fixed $\ol{M} = (M_0,\ldots,M_k)$ and $\ol{N} = (N_0,\ldots,N_k)$, we let
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$FG^n_{\ol{M}\ol{N}}$ denote the topological space of all $n$-dimensional fat graphs as above.
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(Note that in different parts of $FG^n_{\ol{M}\ol{N}}$ the $M_i$'s and $N_i$'s
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are ordered differently.)
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The topology comes from the spaces
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\[
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	\Homeo(M_0\to R_1\cup M_1)\times \Homeo(R_1\cup N_1\to R_2\cup M_2)\times
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			\cdots\times \Homeo(R_k\cup N_k\to N_0)
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\]
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and the above equivalence relations.
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We will denote the typical element of $FG^n_{\ol{M}\ol{N}}$ by $\ol{f} = (f_0,\ldots,f_k)$.
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\medskip
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%The little $n{+}1$-ball operad injects into the $n$-FG operad.
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The $n$-FG operad contains the little $n{+}1$-ball operad.
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Roughly speaking, given a configuration of $k$ little $n{+}1$-balls in the standard
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$n{+}1$-ball, we fiber the complement of the balls by vertical intervals
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and let $M_i$ [$N_i$] be the southern [northern] hemisphere of the $i$-th ball.
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More precisely, let $x_0,\ldots,x_n$ be the coordinates of $\r^{n+1}$.
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Let $z$ be a point of the $k$-th space of the little $n{+}1$-ball operad, with
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little balls $D_1,\ldots,D_k$ inside the standard $n{+}1$-ball.
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We assume the $D_i$'s are ordered according to the $x_n$ coordinate of their centers.
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Let $\pi:\r^{n+1}\to \r^n$ be the projection corresponding to $x_n$.
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Let $B\sub\r^n$ be the standard $n$-ball.
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Let $M_i$ and $N_i$ be $B$ for all $i$.
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Identify $\pi(D_i)$ with $B$ (a.k.a.\ $M_i$ or $N_i$) via translations and dilations (no rotations).
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Let $R_i = B\setmin \pi(D_i)$.
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Let $f_i = \rm{id}$ for all $i$.
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We have now defined a map from the little $n{+}1$-ball operad to the $n$-FG operad,
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with contractible fibers.
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(The fibers correspond to moving the $D_i$'s in the $x_n$ direction without changing their ordering.)
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\nn{issue: we've described this by varying the $R_i$'s, but above we emphasize varying the $f_i$'s.
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does this need more explanation?}
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Another familiar subspace of the $n$-FG operad is $\Homeo(M\to N)$, which corresponds to 
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case $k=0$ (no holes).
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\medskip
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Let $\ol{f} \in FG^n_{\ol{M}\ol{N}}$.
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Let $\hom(\bc_*(M_i), \bc_*(N_i))$ denote the morphisms from $\bc_*(M_i)$ to $\bc_*(N_i)$,
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as modules of the $A_\infty$ 1-category $\bc_*(E_i)$.
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We define a map
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\[
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	p(\ol{f}): \hom(\bc_*(M_1), \bc_*(N_1))\ot\cdots\ot\hom(\bc_*(M_k), \bc_*(N_k))
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				\to \hom(\bc_*(M_0), \bc_*(N_0)) .
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\]
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Given $\alpha_i\in\hom(\bc_*(M_i), \bc_*(N_i))$, we define $p(\ol{f}$) to be the composition
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\[
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	\bc_*(M_0)  \stackrel{f_0}{\to} \bc_*(R_1\cup M_1)
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				 \stackrel{\id\ot\alpha_1}{\to} \bc_*(R_1\cup N_1)
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				 \stackrel{f_1}{\to} \bc_*(R_2\cup M_2) \stackrel{\id\ot\alpha_2}{\to}
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				 \cdots  \stackrel{\id\ot\alpha_k}{\to} \bc_*(R_k\cup N_k)
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				 \stackrel{f_k}{\to} \bc_*(N_0)
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\]
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(Recall that the maps $\id\ot\alpha_i$ were defined in \nn{need ref}.)
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It is easy to check that the above definition is compatible with the equivalence relations
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and also the operad structure.
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We can reinterpret the above as a chain map
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\[
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	p: C_0(FG^n_{\ol{M}\ol{N}})\ot \hom(\bc_*(M_1), \bc_*(N_1))\ot\cdots\ot\hom(\bc_*(M_k), \bc_*(N_k))
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				\to \hom(\bc_*(M_0), \bc_*(N_0)) .
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\]
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The main result of this section is that this chain map extends to the full singular
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chain complex $C_*(FG^n_{\ol{M}\ol{N}})$.
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\begin{prop}
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\label{prop:deligne}
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There is a collection of chain maps
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\[
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	C_*(FG^n_{\overline{M}, \overline{N}})\otimes \hom(\bc_*(M_1), \bc_*(N_1))\otimes\cdots\otimes 
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\hom(\bc_*(M_{k}), \bc_*(N_{k})) \to  \hom(\bc_*(M_0), \bc_*(N_0))
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\]
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which satisfy the operad compatibility conditions.
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On $C_0(FG^n_{\ol{M}\ol{N}})$ this agrees with the chain map $p$ defined above.
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When $k=0$, this coincides with the $C_*(\Homeo(M_0\to N_0))$ action of Section \ref{sec:evaluation}.
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\end{prop}
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If, in analogy to Hochschild cochains, we define elements of $\hom(M, N)$
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to be ``blob cochains", we can summarize the above proposition by saying that the $n$-FG operad acts on
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blob cochains.
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As noted above, the $n$-FG operad contains the little $n{+}1$-ball operad, so this constitutes
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a higher dimensional version of the Deligne conjecture for Hochschild cochains and the little 2-disk operad.
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\nn{...}
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\nn{maybe point out that even for $n=1$ there's something new here.}