pnas/pnas.tex
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   210 Thus we can have the simplicity of strict associativity in exchange for more morphisms.
   210 Thus we can have the simplicity of strict associativity in exchange for more morphisms.
   211 We wish to imitate this strategy in higher categories.
   211 We wish to imitate this strategy in higher categories.
   212 Because we are mainly interested in the case of strong duality, we replace the intervals $[0,r]$ not with
   212 Because we are mainly interested in the case of strong duality, we replace the intervals $[0,r]$ not with
   213 a product of $k$ intervals \nn{cf xxxx} but rather with any $k$-ball, that is, any $k$-manifold which is homeomorphic
   213 a product of $k$ intervals \nn{cf xxxx} but rather with any $k$-ball, that is, any $k$-manifold which is homeomorphic
   214 to the standard $k$-ball $B^k$.
   214 to the standard $k$-ball $B^k$.
   215 \nn{maybe add that in addition we want funtoriality}
   215 \nn{maybe add that in addition we want functoriality}
       
   216 
       
   217 \nn{say something about different flavors of balls; say it here? later?}
   216 
   218 
   217 \begin{axiom}[Morphisms]
   219 \begin{axiom}[Morphisms]
   218 \label{axiom:morphisms}
   220 \label{axiom:morphisms}
   219 For each $0 \le k \le n$, we have a functor $\cC_k$ from 
   221 For each $0 \le k \le n$, we have a functor $\cC_k$ from 
   220 the category of $k$-balls and 
   222 the category of $k$-balls and 
   221 homeomorphisms to the category of sets and bijections.
   223 homeomorphisms to the category of sets and bijections.
   222 \end{axiom}
   224 \end{axiom}
   223 
   225 
   224 
   226 Note that the functoriality in the above axiom allows us to operate via
   225 
   227 
   226 \begin{lem}
   228 Next we consider domains and ranges of $k$-morphisms.
   227 \label{lem:spheres}
   229 Because we assume strong duality, it doesn't make much sense to subdivide the boundary of a morphism
   228 For each $1 \le k \le n$, we have a functor $\cl{\cC}_{k-1}$ from 
   230 into domain and range --- the duality operations can convert domain to range and vice-versa.
   229 the category of $k{-}1$-spheres and 
   231 Instead, we will use a unified domain/range, which we will call a ``boundary".
   230 homeomorphisms to the category of sets and bijections.
   232 
   231 \end{lem}
   233 In order to state the axiom for boundaries, we need to extend the functors $\cC_k$
       
   234 of $k$-balls to functors $\cl{\cC}_{k-1}$ of $k$-spheres.
       
   235 This extension is described in xxxx below.
       
   236 
       
   237 %\begin{lem}
       
   238 %\label{lem:spheres}
       
   239 %For each $1 \le k \le n$, we have a functor $\cl{\cC}_{k-1}$ from 
       
   240 %the category of $k{-}1$-spheres and 
       
   241 %homeomorphisms to the category of sets and bijections.
       
   242 %\end{lem}
   232 
   243 
   233 \begin{axiom}[Boundaries]\label{nca-boundary}
   244 \begin{axiom}[Boundaries]\label{nca-boundary}
   234 For each $k$-ball $X$, we have a map of sets $\bd: \cC_k(X)\to \cl{\cC}_{k-1}(\bd X)$.
   245 For each $k$-ball $X$, we have a map of sets $\bd: \cC_k(X)\to \cl{\cC}_{k-1}(\bd X)$.
   235 These maps, for various $X$, comprise a natural transformation of functors.
   246 These maps, for various $X$, comprise a natural transformation of functors.
   236 \end{axiom}
   247 \end{axiom}
   358 \todo{maps to a space, string diagrams}
   369 \todo{maps to a space, string diagrams}
   359 
   370 
   360 \subsection{The blob complex}
   371 \subsection{The blob complex}
   361 \subsubsection{Decompositions of manifolds}
   372 \subsubsection{Decompositions of manifolds}
   362 
   373 
       
   374 \nn{KW: I'm inclined to suppress all discussion of the subtleties of decompositions.
       
   375 Maybe just a single remark that we are omitting some details which appear in our
       
   376 longer paper.}
       
   377 
   363 A \emph{ball decomposition} of $W$ is a 
   378 A \emph{ball decomposition} of $W$ is a 
   364 sequence of gluings $M_0\to M_1\to\cdots\to M_m = W$ such that $M_0$ is a disjoint union of balls
   379 sequence of gluings $M_0\to M_1\to\cdots\to M_m = W$ such that $M_0$ is a disjoint union of balls
   365 $\du_a X_a$ and each $M_i$ is a manifold.
   380 $\du_a X_a$ and each $M_i$ is a manifold.
   366 If $X_a$ is some component of $M_0$, its image in $W$ need not be a ball; $\bd X_a$ may have been glued to itself.
   381 If $X_a$ is some component of $M_0$, its image in $W$ need not be a ball; $\bd X_a$ may have been glued to itself.
   367 A {\it permissible decomposition} of $W$ is a map
   382 A {\it permissible decomposition} of $W$ is a map
   440 
   455 
   441 \section{Properties of the blob complex}
   456 \section{Properties of the blob complex}
   442 \subsection{Formal properties}
   457 \subsection{Formal properties}
   443 \label{sec:properties}
   458 \label{sec:properties}
   444 The blob complex enjoys the following list of formal properties.
   459 The blob complex enjoys the following list of formal properties.
       
   460 
       
   461 The proofs of the first three properties are immediate from the definitions.
   445 
   462 
   446 \begin{property}[Functoriality]
   463 \begin{property}[Functoriality]
   447 \label{property:functoriality}%
   464 \label{property:functoriality}%
   448 The blob complex is functorial with respect to homeomorphisms.
   465 The blob complex is functorial with respect to homeomorphisms.
   449 That is, 
   466 That is, 
   489 associated by the system of fields $\cF$ to balls.
   506 associated by the system of fields $\cF$ to balls.
   490 \begin{equation*}
   507 \begin{equation*}
   491 \xymatrix{\bc_*(B^n;\cF) \ar[r]^(0.4){\iso}_(0.4){\text{qi}} & H_0(\bc_*(B^n;\cF)) \ar[r]^(0.6)\iso & A_\cF(B^n)}
   508 \xymatrix{\bc_*(B^n;\cF) \ar[r]^(0.4){\iso}_(0.4){\text{qi}} & H_0(\bc_*(B^n;\cF)) \ar[r]^(0.6)\iso & A_\cF(B^n)}
   492 \end{equation*}
   509 \end{equation*}
   493 \end{property}
   510 \end{property}
       
   511 
       
   512 \begin{proof}(Sketch)
       
   513 For $k\ge 1$, the contracting homotopy sends a $k$-blob diagram to the $(k{+}1)$-blob diagram
       
   514 obtained by adding an outer $(k{+}1)$-st blob consisting of all $B^n$.
       
   515 For $k=0$ we choose a splitting $s: H_0(\bc_*(B^n)) \to \bc_0(B^n)$ and send 
       
   516 $x\in \bc_0(B^n)$ to $x - s([x])$, where $[x]$ denotes the image of $x$ in $H_0(\bc_*(B^n))$.
       
   517 \end{proof}
   494 
   518 
   495 \nn{Properties \ref{property:functoriality} will be immediate from the definition given in
   519 \nn{Properties \ref{property:functoriality} will be immediate from the definition given in
   496 \S \ref{sec:blob-definition}, and we'll recall it at the appropriate point there.
   520 \S \ref{sec:blob-definition}, and we'll recall it at the appropriate point there.
   497 Properties \ref{property:disjoint-union}, \ref{property:gluing-map} and 
   521 Properties \ref{property:disjoint-union}, \ref{property:gluing-map} and 
   498 \ref{property:contractibility} are established in \S \ref{sec:basic-properties}.}
   522 \ref{property:contractibility} are established in \S \ref{sec:basic-properties}.}