text/tqftreview.tex
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   211 \]
   211 \]
   212 in the case that $X = X_1 \du X_2$, with $x_i \in \cC(X_i)$.
   212 in the case that $X = X_1 \du X_2$, with $x_i \in \cC(X_i)$.
   213 
   213 
   214 \medskip
   214 \medskip
   215 
   215 
       
   216 
   216 Using the functoriality and product field properties above, together
   217 Using the functoriality and product field properties above, together
   217 with boundary collar homeomorphisms of manifolds, we can define 
   218 with boundary collar homeomorphisms of manifolds, we can define 
   218 {\it collar maps} $\cC(M)\to \cC(M)$.
   219 {\it collar maps} $\cC(M)\to \cC(M)$.
   219 Let $M$ be an $n$-manifold and $Y \subset \bd M$ be a codimension zero submanifold
   220 Let $M$ be an $n$-manifold and $Y \subset \bd M$ be a codimension zero submanifold
   220 of $\bd M$.
   221 of $\bd M$.
   229 can be thought of (informally) as the limit of homeomorphisms
   230 can be thought of (informally) as the limit of homeomorphisms
   230 which expand an infinitesimally thin collar neighborhood of $Y$ to a thicker
   231 which expand an infinitesimally thin collar neighborhood of $Y$ to a thicker
   231 collar neighborhood.
   232 collar neighborhood.
   232 
   233 
   233 
   234 
   234 % all this linearizing stuff is unnecessary, I think
       
   235 \noop{
       
   236 
       
   237 \nn{the following discussion of linearizing fields is kind of lame.
       
   238 maybe just assume things are already linearized.}
       
   239 
       
   240 \nn{remark that if top dimensional fields are not already linear
       
   241 then we will soon linearize them(?)}
       
   242 
       
   243 For top dimensional ($n$-dimensional) manifolds, we're actually interested
       
   244 in the linearized space of fields.
       
   245 By default, define $\lf(X) = \c[\cC(X)]$; that is, $\lf(X)$ is
       
   246 the vector space of finite
       
   247 linear combinations of fields on $X$.
       
   248 If $X$ has boundary, we of course fix a boundary condition: $\lf(X; a) = \c[\cC(X; a)]$.
       
   249 Thus the restriction (to boundary) maps are well defined because we never
       
   250 take linear combinations of fields with differing boundary conditions.
       
   251 
       
   252 In some cases we don't linearize the default way; instead we take the
       
   253 spaces $\lf(X; a)$ to be part of the data for the system of fields.
       
   254 In particular, for fields based on linear $n$-category pictures we linearize as follows.
       
   255 Define $\lf(X; a) = \c[\cC(X; a)]/K$, where $K$ is the space generated by
       
   256 obvious relations on 0-cell labels.
       
   257 More specifically, let $L$ be a cell decomposition of $X$
       
   258 and let $p$ be a 0-cell of $L$.
       
   259 Let $\alpha_c$ and $\alpha_d$ be two labelings of $L$ which are identical except that
       
   260 $\alpha_c$ labels $p$ by $c$ and $\alpha_d$ labels $p$ by $d$.
       
   261 Then the subspace $K$ is generated by things of the form
       
   262 $\lambda \alpha_c + \alpha_d - \alpha_{\lambda c + d}$, where we leave it to the reader
       
   263 to infer the meaning of $\alpha_{\lambda c + d}$.
       
   264 Note that we are still assuming that $n$-categories have linear spaces of $n$-morphisms.
       
   265 
       
   266 \nn{Maybe comment further: if there's a natural basis of morphisms, then no need;
       
   267 will do something similar below; in general, whenever a label lives in a linear
       
   268 space we do something like this; ? say something about tensor
       
   269 product of all the linear label spaces?  Yes:}
       
   270 
       
   271 For top dimensional ($n$-dimensional) manifolds, we linearize as follows.
       
   272 Define an ``almost-field" to be a field without labels on the 0-cells.
       
   273 (Recall that 0-cells are labeled by $n$-morphisms.)
       
   274 To each unlabeled 0-cell in an almost field there corresponds a (linear) $n$-morphism
       
   275 space determined by the labeling of the link of the 0-cell.
       
   276 (If the 0-cell were labeled, the label would live in this space.)
       
   277 We associate to each almost-labeling the tensor product of these spaces (one for each 0-cell).
       
   278 We now define $\lf(X; a)$ to be the direct sum over all almost labelings of the
       
   279 above tensor products.
       
   280 
       
   281 } % end \noop
       
   282 
   235 
   283 
   236 
   284 \subsection{Systems of fields from \texorpdfstring{$n$}{n}-categories}
   237 \subsection{Systems of fields from \texorpdfstring{$n$}{n}-categories}
   285 \label{sec:example:traditional-n-categories(fields)}
   238 \label{sec:example:traditional-n-categories(fields)}
   286 We now describe in more detail Example \ref{ex:traditional-n-categories(fields)}, 
   239 We now describe in more detail Example \ref{ex:traditional-n-categories(fields)},