text/intro.tex
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     9 \item When $\cC$ is the polynomial algebra $k[t]$, thought of as an n-category (see \S \ref{sec:comm_alg}), we have 
     9 \item When $\cC$ is the polynomial algebra $k[t]$, thought of as an n-category (see \S \ref{sec:comm_alg}), we have 
    10 that $\bc_*(M; k[t])$ is homotopy equivalent to $C_*(\Sigma^\infty(M), k)$, the singular chains
    10 that $\bc_*(M; k[t])$ is homotopy equivalent to $C_*(\Sigma^\infty(M), k)$, the singular chains
    11 on the configurations space of unlabeled points in $M$.
    11 on the configurations space of unlabeled points in $M$.
    12 %$$H_*(\bc_*(M; k[t])) = H^{\text{sing}}_*(\Delta^\infty(M), k).$$ 
    12 %$$H_*(\bc_*(M; k[t])) = H^{\text{sing}}_*(\Delta^\infty(M), k).$$ 
    13 \end{itemize}
    13 \end{itemize}
    14 The blob complex has good formal properties, summarized in \S \ref{sec:properties}. These include an action of $\CD{M}$, 
    14 The blob complex definition is motivated by the desire for a derived analogue of the usual TQFT Hilbert space (replacing quotient of fields by local relations with some sort of resolution), 
    15 \nn{maybe replace Diff with Homeo?}
       
    16 extending the usual $\Diff(M)$ action on the TQFT space $H_0$ (see Property \ref{property:evaluation}) and a gluing formula allowing calculations by cutting manifolds into smaller parts (see Property \ref{property:gluing}).
       
    17 
       
    18 The blob complex definition is motivated by the desire for a `derived' analogue of the usual TQFT Hilbert space (replacing quotient of fields by local relations with some sort of `resolution'), 
       
    19 \nn{are the quotes around `derived' and `resolution' necessary?}
       
    20 and for a generalization of Hochschild homology to higher $n$-categories. We would also like to be able to talk about $\CM{M}{T}$ when $T$ is an $n$-category rather than a manifold. The blob complex allows us to do all of these! More detailed motivations are described in \S \ref{sec:motivations}.
    15 and for a generalization of Hochschild homology to higher $n$-categories. We would also like to be able to talk about $\CM{M}{T}$ when $T$ is an $n$-category rather than a manifold. The blob complex allows us to do all of these! More detailed motivations are described in \S \ref{sec:motivations}.
       
    16 
       
    17 The blob complex has good formal properties, summarized in \S \ref{sec:properties}. These include an action of $\CH{M}$, 
       
    18 extending the usual $\Homeo(M)$ action on the TQFT space $H_0$ (see Property \ref{property:evaluation}) and a gluing formula allowing calculations by cutting manifolds into smaller parts (see Property \ref{property:gluing}).
    21 
    19 
    22 We expect applications of the blob complex to contact topology and Khovanov homology but do not address these in this paper. See \S \ref{sec:future} for slightly more detail.
    20 We expect applications of the blob complex to contact topology and Khovanov homology but do not address these in this paper. See \S \ref{sec:future} for slightly more detail.
    23 
    21 
    24 \subsubsection{Structure of the paper}
    22 \subsubsection{Structure of the paper}
    25 The three subsections of the introduction explain our motivations in defining the blob complex (see \S \ref{sec:motivations}), summarise the formal properties of the blob complex (see \S \ref{sec:properties}) and outline anticipated future directions and applications (see \S \ref{sec:future}).
    23 The three subsections of the introduction explain our motivations in defining the blob complex (see \S \ref{sec:motivations}), summarise the formal properties of the blob complex (see \S \ref{sec:properties}) and outline anticipated future directions and applications (see \S \ref{sec:future}).
    27 The first part of the paper (sections \S \ref{sec:fields}---\S \ref{sec:evaluation}) gives the definition of the blob complex, and establishes some of its properties. There are many alternative definitions of $n$-categories, and part of our difficulty defining the blob complex is simply explaining what we mean by an ``$n$-category with strong duality'' as one of the inputs. At first we entirely avoid this problem by introducing the notion of a `system of fields', and define the blob complex associated to an $n$-manifold and an $n$-dimensional system of fields. We sketch the construction of a system of fields from a $1$-category or from a pivotal $2$-category.
    25 The first part of the paper (sections \S \ref{sec:fields}---\S \ref{sec:evaluation}) gives the definition of the blob complex, and establishes some of its properties. There are many alternative definitions of $n$-categories, and part of our difficulty defining the blob complex is simply explaining what we mean by an ``$n$-category with strong duality'' as one of the inputs. At first we entirely avoid this problem by introducing the notion of a `system of fields', and define the blob complex associated to an $n$-manifold and an $n$-dimensional system of fields. We sketch the construction of a system of fields from a $1$-category or from a pivotal $2$-category.
    28 
    26 
    29 Nevertheless, when we attempt to establish all of the observed properties of the blob complex, we find this situation unsatisfactory. Thus, in the second part of the paper (section \S \ref{sec:ncats}) we pause and give yet another definition of an $n$-category, or rather a definition of an $n$-category with strong duality. (It's not clear that we could remove the duality conditions from our definition, even if we wanted to.) We call these ``topological $n$-categories'', to differentiate them from previous versions. Moreover, we find that we need analogous $A_\infty$ $n$-categories, and we define these as well following very similar axioms.
    27 Nevertheless, when we attempt to establish all of the observed properties of the blob complex, we find this situation unsatisfactory. Thus, in the second part of the paper (section \S \ref{sec:ncats}) we pause and give yet another definition of an $n$-category, or rather a definition of an $n$-category with strong duality. (It's not clear that we could remove the duality conditions from our definition, even if we wanted to.) We call these ``topological $n$-categories'', to differentiate them from previous versions. Moreover, we find that we need analogous $A_\infty$ $n$-categories, and we define these as well following very similar axioms.
    30 
    28 
    31 \nn{Not sure that the next para is appropriate here}
    29 \nn{Not sure that the next para is appropriate here}
    32 The basic idea is that each potential definition of an $n$-category makes a choice about the `shape' of morphisms. We try to be as lax as possible; a topological $n$-category associates a vector space to every $B$ diffeomorphic to the $n$-ball. This vector spaces glue together associatively. For an $A_\infty$ $n$-category, we instead associate a chain complex to each such $B$. We require that diffeomorphisms (or the complex of singular chains of diffeomorphisms in the $A_\infty$ case) act. The axioms for an $A_\infty$ $n$-category are designed to capture two main examples: the blob complexes of $n$-balls, using a topological $n$-category, and the complex $\CM{-}{X}$ of maps to a fixed target space $X$.
    30 The basic idea is that each potential definition of an $n$-category makes a choice about the `shape' of morphisms. We try to be as lax as possible; a topological $n$-category associates a vector space to every $B$ homeomorphic to the $n$-ball. This vector spaces glue together associatively. For an $A_\infty$ $n$-category, we instead associate a chain complex to each such $B$. We require that homeomorphisms (or the complex of singular chains of homeomorphisms in the $A_\infty$ case) act. The axioms for an $A_\infty$ $n$-category are designed to capture two main examples: the blob complexes of $n$-balls, using a topological $n$-category, and the complex $\CM{-}{X}$ of maps to a fixed target space $X$.
    33 \nn{we might want to make our choice of notation here ($B$, $X$) consistent with later sections ($X$, $T$), or vice versa}
    31 \nn{we might want to make our choice of notation here ($B$, $X$) consistent with later sections ($X$, $T$), or vice versa}
    34 
    32 
    35 In  \S \ref{sec:ainfblob} we explain how to construct a system of fields from a topological $n$-category, and give an alternative definition of the blob complex for an $n$-manifold and an $A_\infty$ $n$-category. Using these definitions, we show how to use the blob complex to `resolve' any topological $n$-category as an $A_\infty$ $n$-category, and relate the first and second definitions of the blob complex. We use the blob complex for $A_\infty$ $n$-categories to establish important properties of the blob complex (in both variants), in particular the `gluing formula' of Property \ref{property:gluing} below.
    33 In  \S \ref{sec:ainfblob} we explain how to construct a system of fields from a topological $n$-category, and give an alternative definition of the blob complex for an $n$-manifold and an $A_\infty$ $n$-category. Using these definitions, we show how to use the blob complex to `resolve' any topological $n$-category as an $A_\infty$ $n$-category, and relate the first and second definitions of the blob complex. We use the blob complex for $A_\infty$ $n$-categories to establish important properties of the blob complex (in both variants), in particular the `gluing formula' of Property \ref{property:gluing} below.
    36 
    34 
    37 \nn{KW: the previous two paragraphs seem a little awkward to me, but I don't presently have a good idea for fixing them.}
    35 \nn{KW: the previous two paragraphs seem a little awkward to me, but I don't presently have a good idea for fixing them.}
    38 
    36 
    39 Finally, later sections address other topics. Section \S \ref{sec:comm_alg} describes the blob complex when $\cC$ is a commutative algebra, thought of as a topological $n$-category, in terms of the topology of $M$. Section \S \ref{sec:deligne} states (and in a later edition of this paper, hopefully proves) a generalisation of the Deligne conjecture (that the little discs operad acts on Hochschild cohomology) in terms of the blob complex. The appendixes prove technical results about $\CD{M}$, and make connections between our definitions of $n$-categories and familar definitions for $n=1$ and $n=2$, as well as relating the $n=1$ case of our $A_\infty$ $n$-categories with usual $A_\infty$ algebras.
    37 Finally, later sections address other topics. Section \S \ref{sec:comm_alg} describes the blob complex when $\cC$ is a commutative algebra, thought of as a topological $n$-category, in terms of the topology of $M$. Section \S \ref{sec:deligne} states (and in a later edition of this paper, hopefully proves) a generalisation of the Deligne conjecture (that the little discs operad acts on Hochschild cohomology) in terms of the blob complex. The appendixes prove technical results about $\CH{M}$, and make connections between our definitions of $n$-categories and familar definitions for $n=1$ and $n=2$, as well as relating the $n=1$ case of our $A_\infty$ $n$-categories with usual $A_\infty$ algebras.
    40 
    38 
    41 
    39 
    42 \nn{some more things to cover in the intro}
    40 \nn{some more things to cover in the intro}
    43 \begin{itemize}
    41 \begin{itemize}
    44 \item related: we are being unsophisticated from a homotopy theory point of
    42 \item related: we are being unsophisticated from a homotopy theory point of
    56 We will briefly sketch our original motivation for defining the blob complex.
    54 We will briefly sketch our original motivation for defining the blob complex.
    57 \nn{this is adapted from an old draft of the intro; it needs further modification
    55 \nn{this is adapted from an old draft of the intro; it needs further modification
    58 in order to better integrate it into the current intro.}
    56 in order to better integrate it into the current intro.}
    59 
    57 
    60 As a starting point, consider TQFTs constructed via fields and local relations.
    58 As a starting point, consider TQFTs constructed via fields and local relations.
    61 (See Section \ref{sec:tqftsviafields} or \cite{kwtqft}.)
    59 (See Section \ref{sec:tqftsviafields} or \cite{kw:tqft}.)
    62 This gives a satisfactory treatment for semisimple TQFTs
    60 This gives a satisfactory treatment for semisimple TQFTs
    63 (i.e.\ TQFTs for which the cylinder 1-category associated to an
    61 (i.e.\ TQFTs for which the cylinder 1-category associated to an
    64 $n{-}1$-manifold $Y$ is semisimple for all $Y$).
    62 $n{-}1$-manifold $Y$ is semisimple for all $Y$).
    65 
    63 
    66 For non-semiemple TQFTs, this approach is less satisfactory.
    64 For non-semi-simple TQFTs, this approach is less satisfactory.
    67 Our main motivating example (though we will not develop it in this paper)
    65 Our main motivating example (though we will not develop it in this paper)
    68 is the (decapitated) $4{+}1$-dimensional TQFT associated to Khovanov homology.
    66 is the (decapitated) $4{+}1$-dimensional TQFT associated to Khovanov homology.
    69 It associates a bigraded vector space $A_{Kh}(W^4, L)$ to a 4-manifold $W$ together
    67 It associates a bigraded vector space $A_{Kh}(W^4, L)$ to a 4-manifold $W$ together
    70 with a link $L \subset \bd W$.
    68 with a link $L \subset \bd W$.
    71 The original Khovanov homology of a link in $S^3$ is recovered as $A_{Kh}(B^4, L)$.
    69 The original Khovanov homology of a link in $S^3$ is recovered as $A_{Kh}(B^4, L)$.
    72 
    70 
    73 How would we go about computing $A_{Kh}(W^4, L)$?
    71 How would we go about computing $A_{Kh}(W^4, L)$?
    74 For $A_{Kh}(B^4, L)$, the main tool is the exact triangle (long exact sequence)
    72 For $A_{Kh}(B^4, L)$, the main tool is the exact triangle (long exact sequence)
    75 \nn{... $L_1, L_2, L_3$}.
    73 relating resolutions of a crossing.
    76 Unfortunately, the exactness breaks if we glue $B^4$ to itself and attempt
    74 Unfortunately, the exactness breaks if we glue $B^4$ to itself and attempt
    77 to compute $A_{Kh}(S^1\times B^3, L)$.
    75 to compute $A_{Kh}(S^1\times B^3, L)$.
    78 According to the gluing theorem for TQFTs-via-fields, gluing along $B^3 \subset \bd B^4$
    76 According to the gluing theorem for TQFTs-via-fields, gluing along $B^3 \subset \bd B^4$
    79 corresponds to taking a coend (self tensor product) over the cylinder category
    77 corresponds to taking a coend (self tensor product) over the cylinder category
    80 associated to $B^3$ (with appropriate boundary conditions).
    78 associated to $B^3$ (with appropriate boundary conditions).
   111 $\bc_1$ is linear combinations of local relations on $W$,
   109 $\bc_1$ is linear combinations of local relations on $W$,
   112 $\bc_2$ is linear combinations of relations amongst relations on $W$,
   110 $\bc_2$ is linear combinations of relations amongst relations on $W$,
   113 and so on.
   111 and so on.
   114 
   112 
   115 None of the above ideas depend on the details of the Khovanov homology example,
   113 None of the above ideas depend on the details of the Khovanov homology example,
   116 so we develop the general theory in the paper and postpone specific applications
   114 so we develop the general theory in this paper and postpone specific applications
   117 to later papers.
   115 to later papers.
   118 
   116 
   119 
   117 
   120 
   118 
   121 \subsection{Formal properties}
   119 \subsection{Formal properties}
   184 \begin{equation*}
   182 \begin{equation*}
   185 \xymatrix{\bc_*^{\cC}(S^1) \ar[r]^{\iso}_{\text{qi}} & \HC_*(\cC)}
   183 \xymatrix{\bc_*^{\cC}(S^1) \ar[r]^{\iso}_{\text{qi}} & \HC_*(\cC)}
   186 \end{equation*}
   184 \end{equation*}
   187 \end{property}
   185 \end{property}
   188 
   186 
   189 Here $\CD{X}$ is the singular chain complex of the space of diffeomorphisms of $X$, fixed on $\bdy X$.
   187 Here $\CH{X}$ is the singular chain complex of the space of homeomorphisms of $X$, fixed on $\bdy X$.
   190 \begin{property}[$C_*(\Diff(-))$ action]
   188 \begin{property}[$C_*(\Homeo(-))$ action]
   191 \label{property:evaluation}%
   189 \label{property:evaluation}%
   192 There is a chain map
   190 There is a chain map
   193 \begin{equation*}
   191 \begin{equation*}
   194 \ev_X: \CD{X} \tensor \bc_*(X) \to \bc_*(X).
   192 \ev_X: \CH{X} \tensor \bc_*(X) \to \bc_*(X).
   195 \end{equation*}
   193 \end{equation*}
   196 
   194 
   197 Restricted to $C_0(\Diff(X))$ this is just the action of diffeomorphisms described in Property \ref{property:functoriality}. Further, for
   195 Restricted to $C_0(\Homeo(X))$ this is just the action of homeomorphisms described in Property \ref{property:functoriality}. Further, for
   198 any codimension $1$-submanifold $Y \subset X$ dividing $X$ into $X_1 \cup_Y X_2$, the following diagram
   196 any codimension $1$-submanifold $Y \subset X$ dividing $X$ into $X_1 \cup_Y X_2$, the following diagram
   199 (using the gluing maps described in Property \ref{property:gluing-map}) commutes.
   197 (using the gluing maps described in Property \ref{property:gluing-map}) commutes.
   200 \begin{equation*}
   198 \begin{equation*}
   201 \xymatrix{
   199 \xymatrix{
   202      \CD{X} \otimes \bc_*(X) \ar[r]^{\ev_X}    & \bc_*(X) \\
   200      \CH{X} \otimes \bc_*(X) \ar[r]^{\ev_X}    & \bc_*(X) \\
   203      \CD{X_1} \otimes \CD{X_2} \otimes \bc_*(X_1) \otimes \bc_*(X_2)
   201      \CH{X_1} \otimes \CH{X_2} \otimes \bc_*(X_1) \otimes \bc_*(X_2)
   204         \ar@/_4ex/[r]_{\ev_{X_1} \otimes \ev_{X_2}}  \ar[u]^{\gl^{\Diff}_Y \otimes \gl_Y}  &
   202         \ar@/_4ex/[r]_{\ev_{X_1} \otimes \ev_{X_2}}  \ar[u]^{\gl^{\Homeo}_Y \otimes \gl_Y}  &
   205             \bc_*(X_1) \otimes \bc_*(X_2) \ar[u]_{\gl_Y}
   203             \bc_*(X_1) \otimes \bc_*(X_2) \ar[u]_{\gl_Y}
   206 }
   204 }
   207 \end{equation*}
   205 \end{equation*}
   208 \nn{should probably say something about associativity here (or not?)}
   206 \nn{should probably say something about associativity here (or not?)}
   209 \nn{maybe do self-gluing instead of 2 pieces case:}
   207 \nn{maybe do self-gluing instead of 2 pieces case:}
   210 Further, for
   208 Further, for
   211 any codimension $0$-submanifold $Y \sqcup Y^\text{op} \subset \bdy X$ the following diagram
   209 any codimension $0$-submanifold $Y \sqcup Y^\text{op} \subset \bdy X$ the following diagram
   212 (using the gluing maps described in Property \ref{property:gluing-map}) commutes.
   210 (using the gluing maps described in Property \ref{property:gluing-map}) commutes.
   213 \begin{equation*}
   211 \begin{equation*}
   214 \xymatrix@C+2cm{
   212 \xymatrix@C+2cm{
   215      \CD{X \bigcup_Y \selfarrow} \otimes \bc_*(X \bigcup_Y \selfarrow) \ar[r]^<<<<<<<<<<<<{\ev_{(X \bigcup_Y \scalebox{0.5}{\selfarrow})}}    & \bc_*(X \bigcup_Y \selfarrow) \\
   213      \CH{X \bigcup_Y \selfarrow} \otimes \bc_*(X \bigcup_Y \selfarrow) \ar[r]^<<<<<<<<<<<<{\ev_{(X \bigcup_Y \scalebox{0.5}{\selfarrow})}}    & \bc_*(X \bigcup_Y \selfarrow) \\
   216      \CD{X} \otimes \bc_*(X)
   214      \CH{X} \otimes \bc_*(X)
   217         \ar[r]_{\ev_{X}}  \ar[u]^{\gl^{\Diff}_Y \otimes \gl_Y}  &
   215         \ar[r]_{\ev_{X}}  \ar[u]^{\gl^{\Homeo}_Y \otimes \gl_Y}  &
   218             \bc_*(X) \ar[u]_{\gl_Y}
   216             \bc_*(X) \ar[u]_{\gl_Y}
   219 }
   217 }
   220 \end{equation*}
   218 \end{equation*}
   221 \end{property}
   219 \end{property}
   222 
   220 
   238 \begin{property}[Product formula]
   236 \begin{property}[Product formula]
   239 Let $W$ be a $k$-manifold and $Y$ be an $n-k$ manifold. Let $\cC$ be an $n$-category.
   237 Let $W$ be a $k$-manifold and $Y$ be an $n-k$ manifold. Let $\cC$ be an $n$-category.
   240 Let $A_*(Y)$ be the $A_\infty$ $k$-category associated to $Y$ via blob homology (see Property \ref{property:blobs-ainfty}).
   238 Let $A_*(Y)$ be the $A_\infty$ $k$-category associated to $Y$ via blob homology (see Property \ref{property:blobs-ainfty}).
   241 Then
   239 Then
   242 \[
   240 \[
   243 	\bc_*(Y^{n-k}\times W^k, \cC) \simeq \bc_*(W, A_*(Y)) .
   241 	\bc_*(Y\times W, \cC) \simeq \bc_*(W, A_*(Y)) .
   244 \]
   242 \]
   245 Note on the right here we have the version of the blob complex for $A_\infty$ $n$-categories.
   243 Note on the right hand side we have the version of the blob complex for $A_\infty$ $n$-categories.
   246 \end{property}
   244 \end{property}
   247 It seems reasonable to expect a generalization describing an arbitrary fibre bundle. See in particular \S \ref{moddecss} for the framework as such a statement.
   245 It seems reasonable to expect a generalization describing an arbitrary fibre bundle. See in particular \S \ref{moddecss} for the framework as such a statement.
   248 
   246 
   249 \begin{property}[Gluing formula]
   247 \begin{property}[Gluing formula]
   250 \label{property:gluing}%
   248 \label{property:gluing}%
   291 \subsection{Future directions}
   289 \subsection{Future directions}
   292 \label{sec:future}
   290 \label{sec:future}
   293 Throughout, we have resisted the temptation to work in the greatest generality possible (don't worry, it wasn't that hard). 
   291 Throughout, we have resisted the temptation to work in the greatest generality possible (don't worry, it wasn't that hard). 
   294 In most of the places where we say ``set" or ``vector space", any symmetric monoidal category would do.
   292 In most of the places where we say ``set" or ``vector space", any symmetric monoidal category would do.
   295 \nn{maybe make similar remark about chain complexes and $(\infty, 0)$-categories}
   293 \nn{maybe make similar remark about chain complexes and $(\infty, 0)$-categories}
   296 More could be said about finite characteristic (there appears in be $2$-torsion in $\bc_1(S^2, \cC)$ for any spherical $2$-category $\cC$). Much more could be said about other types of manifolds, in particular oriented, $\operatorname{Spin}$ and $\operatorname{Pin}^{\pm}$ manifolds, where boundary issues become more complicated. (We'd recommend thinking about boundaries as germs, rather than just codimension $1$ manifolds.) We've also take the path of least resistance by considering $\operatorname{PL}$ manifolds; there may be some differences for topological manifolds and smooth manifolds.
   294 More could be said about finite characteristic (there appears in be $2$-torsion in $\bc_1(S^2, \cC)$ for any spherical $2$-category $\cC$, for example). Much more could be said about other types of manifolds, in particular oriented, $\operatorname{Spin}$ and $\operatorname{Pin}^{\pm}$ manifolds, where boundary issues become more complicated. (We'd recommend thinking about boundaries as germs, rather than just codimension $1$ manifolds.) We've also take the path of least resistance by considering $\operatorname{PL}$ manifolds; there may be some differences for topological manifolds and smooth manifolds.
   297 
   295 
   298 Many results in Hochschild homology can be understood `topologically' via the blob complex. For example, we expect that the shuffle product on the Hochschild homology of a commutative algebra $A$ simply corresponds to the gluing operation on $\bc_*(S^1 \times [0,1], A)$, but haven't investigated the details.
   296 Many results in Hochschild homology can be understood `topologically' via the blob complex. For example, we expect that the shuffle product on the Hochschild homology of a commutative algebra $A$ simply corresponds to the gluing operation on $\bc_*(S^1 \times [0,1], A)$, but haven't investigated the details.
   299 
   297 
   300 Most importantly, however, \nn{applications!} \nn{$n=2$ cases, contact, Kh}
   298 Most importantly, however, \nn{applications!} \nn{$n=2$ cases, contact, Kh}
   301 
   299