diff -r b5c1a6aec50d -r 08bbcf3ec4d2 text/fields.tex
--- a/text/fields.tex	Wed Oct 28 21:41:53 2009 +0000
+++ /dev/null	Thu Jan 01 00:00:00 1970 +0000
@@ -1,42 +0,0 @@
-\nn{This file is obsolete.}
-
-\todo{beginning of scott's attempt to write down what fields are...}
-
-\newcommand{\manifolds}[1]{\cM_{#1}}
-\newcommand{\closedManifolds}[1]{\cM_{#1}^{\text{closed}}}
-\newcommand{\boundaryConditions}[1]{\cM_{#1}^{\bdy}}
-Let $\manifolds{k}$ be the groupoid of manifolds (possibly with boundary) of dimension $k$ and diffeomorphisms between them. Write
-$\closedManifolds{k}$ for the subgroupoid of closed manifolds. Taking the boundary gives a functor $\bdy : \manifolds{k} \to \closedManifolds{k-1}$.
-Both $\manifolds{k}$ and $\closedManifolds{k}$ are symmetric tensor categories under the operation of disjoint union.
-\begin{defn}
-A \emph{system of fields} is a collection of functors $\cF_k$ associating a `set of fields' to each manifold of dimension at most $n$.
-
-First, there are functors $\cF_k : \closedManifolds{k} \to \Set$ for each $0 \leq k < n$. We ask that these are tensor functors, so they
-take disjoint unions of manifolds to cartesian products of sets. In particular, this means that $\cF_k(\eset)$ is a point; there's only one field
-on the empty manifold of any dimension.
-
-Define the groupoid $\boundaryConditions{k}$ of `manifolds with boundary conditions' as
-\begin{equation*}
-\setc{(Y; c)}{\begin{array}{c} \text{$Y$ a $k$-manifold} \\  c \in \cC_{k-1}(\bdy Y) \end{array}}
-\xymatrix{ \ar@(ru,rd)@<-1ex>[]}
-\set{Y \diffeoto Y'}
-\end{equation*}
-where we think of $f: Y \diffeoto Y'$ as a morphism $(Y; c) \isoto (Y'; \cC_{k-1}(\restrict{f}{\bdy Y})(c))$.
-%
-%The objects are pairs $(Y; c)$ with $Y$ a manifold (possibly with boundary) of dimension $k$ and $c \in \cC_{k-1}(\bdy Y)$
-%a field on the boundary of $Y$. A morphism $(Y; c) \to (Y'; c')$ is any diffeomorphism $f: Y \to Y'$ such that $\cC_{k-1}(\restrict{f}{\bdy Y})(c) = c'$.
-Notice that $\closedManifolds{k}$ is naturally a subgroupoid of $\boundaryConditions{k}$, since a closed manifold has a unique field on its (empty) boundary.
-
-We now ask that the functors $\cF_k$ above extend to functors $\cF_k : \boundaryConditions{k} \to \Set$ for  each $0 \leq k < n$,
-and that there is an extra functor at the top level, $\cF_n : \boundaryConditions{n} \to \Vect$. (Notice that for $n$-manifolds we ask for a vector space, not just a set. This isn't essential for the definition, but we will only be interested in this case hereafter.)
-We still require that these are tensor functors, and so take disjoint unions of manifolds to cartesian products of sets, or tensor products of vector spaces, as appropriate.
-
-\scott{Not sure how to say product fields in this setup.}
-Finally, notice there are functors $- \times I : \manifolds{k} \to \manifolds{k+1}$
-Finally (?) we ask for natural transformations $- \times I : \cC_k \to \cC_{k+1} \compose (- \times I)$. Thus for each pair $(Y^k; c)$ we have a map $\cC_k($
-\end{defn}
-\begin{rem}
-Where the dimension of the manifold is clear, we'll often leave off the subscript on $\cC_k$.
-\end{rem}
-
-\todo{end}
\ No newline at end of file