text/tqftreview.tex
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     2 
     2 
     3 \section{TQFTs via fields}
     3 \section{TQFTs via fields}
     4 \label{sec:fields}
     4 \label{sec:fields}
     5 \label{sec:tqftsviafields}
     5 \label{sec:tqftsviafields}
     6 
     6 
     7 In this section we review the construction of TQFTs from ``topological fields".
     7 In this section we review the notion of a ``system of fields and local relations".
     8 For more details see \cite{kw:tqft}.
     8 For more details see \cite{kw:tqft}. From a system of fields and local relations we can readily construct TQFT invariants of manifolds. This is described in \S \ref{sec:constructing-a-TQFT}. A system of fields is very closely related to an $n$-category. In Example \ref{ex:traditional-n-categories(fields)}, which runs throughout this section, we sketch the construction of a system of fields from an $n$-category. We make this more precise for $n=1$ or $2$ in \S \ref{sec:example:traditional-n-categories(fields)}, and much later, after we've have given our own definition of a `topological $n$-category' in \S \ref{sec:ncats}, we explain precisely how to go back and forth between a topological $n$-category and a system of fields and local relations.
     9 
     9 
    10 We only consider compact manifolds, so if $Y \sub X$ is a closed codimension 0
    10 We only consider compact manifolds, so if $Y \sub X$ is a closed codimension 0
    11 submanifold of $X$, then $X \setmin Y$ implicitly means the closure
    11 submanifold of $X$, then $X \setmin Y$ implicitly means the closure
    12 $\overline{X \setmin Y}$.
    12 $\overline{X \setmin Y}$.
    13 
    13 
    19 $k$ and morphisms homeomorphisms.
    19 $k$ and morphisms homeomorphisms.
    20 (We could equally well work with a different category of manifolds ---
    20 (We could equally well work with a different category of manifolds ---
    21 oriented, topological, smooth, spin, etc. --- but for definiteness we
    21 oriented, topological, smooth, spin, etc. --- but for definiteness we
    22 will stick with unoriented PL.)
    22 will stick with unoriented PL.)
    23 
    23 
    24 %Fix a top dimension $n$, and a symmetric monoidal category $\cS$ whose objects are sets. While reading the definition, you should just think about the case $\cS = \Set$ with cartesian product, until you reach the discussion of a \emph{linear system of fields} later in this section, where $\cS = \Vect$, and \S \ref{sec:homological-fields}, where $\cS = \Kom$.
    24 Fix a symmetric monoidal category $\cS$ whose objects are sets. While reading the definition, you should just think about the cases $\cS = \Set$ or $\cS = \Vect$.
    25 
    25 
    26 A $n$-dimensional {\it system of fields} in $\cS$
    26 A $n$-dimensional {\it system of fields} in $\cS$
    27 is a collection of functors $\cC_k : \cM_k \to \Set$ for $0 \leq k \leq n$
    27 is a collection of functors $\cC_k : \cM_k \to \Set$ for $0 \leq k \leq n$
    28 together with some additional data and satisfying some additional conditions, all specified below.
    28 together with some additional data and satisfying some additional conditions, all specified below.
    29 
    29 
    30 Before finishing the definition of fields, we give two motivating examples
    30 Before finishing the definition of fields, we give two motivating examples of systems of fields.
    31 (actually, families of examples) of systems of fields.
       
    32 
    31 
    33 \begin{example}
    32 \begin{example}
    34 \label{ex:maps-to-a-space(fields)}
    33 \label{ex:maps-to-a-space(fields)}
    35 Fix a target space $B$, and let $\cC(X)$ be the set of continuous maps
    34 Fix a target space $T$, and let $\cC(X)$ be the set of continuous maps
    36 from X to $B$.
    35 from X to $B$.
    37 \end{example}
    36 \end{example}
    38 
    37 
    39 \begin{example}
    38 \begin{example}
    40 \label{ex:traditional-n-categories(fields)}
    39 \label{ex:traditional-n-categories(fields)}
    41 Fix an $n$-category $C$, and let $\cC(X)$ be 
    40 Fix an $n$-category $C$, and let $\cC(X)$ be 
    42 the set of sub-cell-complexes of $X$ with codimension-$j$ cells labeled by
    41 the set of sub-cell-complexes of $X$ with codimension-$j$ cells labeled by
    43 $j$-morphisms of $C$.
    42 $j$-morphisms of $C$.
    44 One can think of such sub-cell-complexes as dual to pasting diagrams for $C$.
    43 One can think of such sub-cell-complexes as dual to pasting diagrams for $C$.
    45 This is described in more detail below.
    44 This is described in more detail in \S \ref{sec:example:traditional-n-categories(fields)}.
    46 \end{example}
    45 \end{example}
    47 
    46 
    48 Now for the rest of the definition of system of fields.
    47 Now for the rest of the definition of system of fields.
    49 \begin{enumerate}
    48 \begin{enumerate}
    50 \item There are boundary restriction maps $\cC_k(X) \to \cC_{k-1}(\bd X)$, 
    49 \item There are boundary restriction maps $\cC_k(X) \to \cC_{k-1}(\bd X)$, 
   142 
   141 
   143 
   142 
   144 \nn{remark that if top dimensional fields are not already linear
   143 \nn{remark that if top dimensional fields are not already linear
   145 then we will soon linearize them(?)}
   144 then we will soon linearize them(?)}
   146 
   145 
       
   146 For top dimensional ($n$-dimensional) manifolds, we're actually interested
       
   147 in the linearized space of fields.
       
   148 By default, define $\lf(X) = \c[\cC(X)]$; that is, $\lf(X)$ is
       
   149 the vector space of finite
       
   150 linear combinations of fields on $X$.
       
   151 If $X$ has boundary, we of course fix a boundary condition: $\lf(X; a) = \c[\cC(X; a)]$.
       
   152 Thus the restriction (to boundary) maps are well defined because we never
       
   153 take linear combinations of fields with differing boundary conditions.
       
   154 
       
   155 In some cases we don't linearize the default way; instead we take the
       
   156 spaces $\lf(X; a)$ to be part of the data for the system of fields.
       
   157 In particular, for fields based on linear $n$-category pictures we linearize as follows.
       
   158 Define $\lf(X; a) = \c[\cC(X; a)]/K$, where $K$ is the space generated by
       
   159 obvious relations on 0-cell labels.
       
   160 More specifically, let $L$ be a cell decomposition of $X$
       
   161 and let $p$ be a 0-cell of $L$.
       
   162 Let $\alpha_c$ and $\alpha_d$ be two labelings of $L$ which are identical except that
       
   163 $\alpha_c$ labels $p$ by $c$ and $\alpha_d$ labels $p$ by $d$.
       
   164 Then the subspace $K$ is generated by things of the form
       
   165 $\lambda \alpha_c + \alpha_d - \alpha_{\lambda c + d}$, where we leave it to the reader
       
   166 to infer the meaning of $\alpha_{\lambda c + d}$.
       
   167 Note that we are still assuming that $n$-categories have linear spaces of $n$-morphisms.
       
   168 
       
   169 \nn{Maybe comment further: if there's a natural basis of morphisms, then no need;
       
   170 will do something similar below; in general, whenever a label lives in a linear
       
   171 space we do something like this; ? say something about tensor
       
   172 product of all the linear label spaces?  Yes:}
       
   173 
       
   174 For top dimensional ($n$-dimensional) manifolds, we linearize as follows.
       
   175 Define an ``almost-field" to be a field without labels on the 0-cells.
       
   176 (Recall that 0-cells are labeled by $n$-morphisms.)
       
   177 To each unlabeled 0-cell in an almost field there corresponds a (linear) $n$-morphism
       
   178 space determined by the labeling of the link of the 0-cell.
       
   179 (If the 0-cell were labeled, the label would live in this space.)
       
   180 We associate to each almost-labeling the tensor product of these spaces (one for each 0-cell).
       
   181 We now define $\lf(X; a)$ to be the direct sum over all almost labelings of the
       
   182 above tensor products.
       
   183 
       
   184 
       
   185 \subsection{Systems of fields from $n$-categories}
       
   186 \label{sec:example:traditional-n-categories(fields)}
   147 We now describe in more detail systems of fields coming from sub-cell-complexes labeled
   187 We now describe in more detail systems of fields coming from sub-cell-complexes labeled
   148 by $n$-category morphisms.
   188 by $n$-category morphisms.
   149 
   189 
   150 Given an $n$-category $C$ with the right sort of duality
   190 Given an $n$-category $C$ with the right sort of duality
   151 (e.g. pivotal 2-category, 1-category with duals, star 1-category, disklike $n$-category),
   191 (e.g. pivotal 2-category, 1-category with duals, star 1-category, disklike $n$-category),
   224 %be treated differently (segregated) from other local relations, but I'm not sure
   264 %be treated differently (segregated) from other local relations, but I'm not sure
   225 %the next definition is the best way to do it}
   265 %the next definition is the best way to do it}
   226 
   266 
   227 \medskip
   267 \medskip
   228 
   268 
   229 For top dimensional ($n$-dimensional) manifolds, we're actually interested
       
   230 in the linearized space of fields.
       
   231 By default, define $\lf(X) = \c[\cC(X)]$; that is, $\lf(X)$ is
       
   232 the vector space of finite
       
   233 linear combinations of fields on $X$.
       
   234 If $X$ has boundary, we of course fix a boundary condition: $\lf(X; a) = \c[\cC(X; a)]$.
       
   235 Thus the restriction (to boundary) maps are well defined because we never
       
   236 take linear combinations of fields with differing boundary conditions.
       
   237 
       
   238 In some cases we don't linearize the default way; instead we take the
       
   239 spaces $\lf(X; a)$ to be part of the data for the system of fields.
       
   240 In particular, for fields based on linear $n$-category pictures we linearize as follows.
       
   241 Define $\lf(X; a) = \c[\cC(X; a)]/K$, where $K$ is the space generated by
       
   242 obvious relations on 0-cell labels.
       
   243 More specifically, let $L$ be a cell decomposition of $X$
       
   244 and let $p$ be a 0-cell of $L$.
       
   245 Let $\alpha_c$ and $\alpha_d$ be two labelings of $L$ which are identical except that
       
   246 $\alpha_c$ labels $p$ by $c$ and $\alpha_d$ labels $p$ by $d$.
       
   247 Then the subspace $K$ is generated by things of the form
       
   248 $\lambda \alpha_c + \alpha_d - \alpha_{\lambda c + d}$, where we leave it to the reader
       
   249 to infer the meaning of $\alpha_{\lambda c + d}$.
       
   250 Note that we are still assuming that $n$-categories have linear spaces of $n$-morphisms.
       
   251 
       
   252 \nn{Maybe comment further: if there's a natural basis of morphisms, then no need;
       
   253 will do something similar below; in general, whenever a label lives in a linear
       
   254 space we do something like this; ? say something about tensor
       
   255 product of all the linear label spaces?  Yes:}
       
   256 
       
   257 For top dimensional ($n$-dimensional) manifolds, we linearize as follows.
       
   258 Define an ``almost-field" to be a field without labels on the 0-cells.
       
   259 (Recall that 0-cells are labeled by $n$-morphisms.)
       
   260 To each unlabeled 0-cell in an almost field there corresponds a (linear) $n$-morphism
       
   261 space determined by the labeling of the link of the 0-cell.
       
   262 (If the 0-cell were labeled, the label would live in this space.)
       
   263 We associate to each almost-labeling the tensor product of these spaces (one for each 0-cell).
       
   264 We now define $\lf(X; a)$ to be the direct sum over all almost labelings of the
       
   265 above tensor products.
       
   266 
   269 
   267 
   270 
   268 
   271 
   269 \subsection{Local relations}
   272 \subsection{Local relations}
   270 \label{sec:local-relations}
   273 \label{sec:local-relations}