# HG changeset patch # User kevin@6e1638ff-ae45-0410-89bd-df963105f760 # Date 1235705381 0 # Node ID 46b5c4f3e83c0e26db40d652faadbd354f5d3b36 # Parent ac5c74fa38d70aa31dba592b2a44c295b466927c finished draft of fields definition; begin to work on local relations definition diff -r ac5c74fa38d7 -r 46b5c4f3e83c blob1.tex --- a/blob1.tex Thu Feb 26 19:01:32 2009 +0000 +++ b/blob1.tex Fri Feb 27 03:29:41 2009 +0000 @@ -319,8 +319,12 @@ \item There are boundary restriction maps $\cC_k(X) \to \cC_{k-1}(\bd X)$, and these maps are a natural transformation between the functors $\cC_k$ and $\cC_{k-1}\circ\bd$. +For $c \in \cC_{k-1}(\bd X)$, we will denote by $\cC_k(X; c)$ the subset of +$\cC(X)$ which restricts to $c$. +In this context, we will call $c$ a boundary condition. \item There are orientation reversal maps $\cC_k(X) \to \cC_k(-X)$, and these maps again comprise a natural transformation of functors. +In addition, the orientation reversal maps are compatible with the boundary restriction maps. \item $\cC_k$ is compatible with the symmetric monoidal structures on $\cM_k$ and sets: $\cC_k(X \du W) \cong \cC_k(X)\times \cC_k(W)$, compatibly with homeomorphisms, restriction to boundary, and orientation reversal. @@ -342,10 +346,36 @@ From the point of view of $X\sgl$ and the image $Y \subset X\sgl$ of the gluing surface, we say that fields in the image of the gluing map are transverse to $Y$ or cuttable along $Y$. -\item Gluing with corners. \nn{...} -\item ``product with $I$" maps $\cC(Y)\to \cC(Y\times I)$; -fiber-preserving homeos of $Y\times I$ act trivially on image -\nn{...} +\item Gluing with corners. +Let $\bd X = Y \cup -Y \cup W$, where $\pm Y$ and $W$ might intersect along their boundaries. +Let $X\sgl$ denote $X$ glued to itself along $\pm Y$. +Note that $\bd X\sgl = W\sgl$, where $W\sgl$ denotes $W$ glued to itself +(without corners) along two copies of $\bd Y$. +Let $c\sgl \in \cC_{k-1}(W\sgl)$ be a be a cuttable field on $W\sgl$ and let +$c \in \cC_{k-1}(W)$ be the cut open version of $c\sgl$. +Let $\cC^c_k(X)$ denote the subset of $\cC(X)$ which restricts to $c$ on $W$. +(This restriction map uses the gluing without corners map above.) +Using the boundary restriction, gluing without corners, and (in one case) orientation reversal +maps, we get two maps $\cC^c_k(X) \to \cC(Y)$, corresponding to the two +copies of $Y$ in $\bd X$. +Let $\Eq^c_Y(\cC_k(X))$ denote the equalizer of these two maps. +Then (here's the axiom/definition part) there is an injective ``gluing" map +\[ + \Eq^c_Y(\cC_k(X)) \hookrightarrow \cC_k(X\sgl, c\sgl) , +\] +and this gluing map is compatible with all of the above structure (actions +of homeomorphisms, boundary restrictions, orientation reversal, disjoint union). +Furthermore, up to homeomorphisms of $X\sgl$ isotopic to the identity, +the gluing map is surjective. +From the point of view of $X\sgl$ and the image $Y \subset X\sgl$ of the +gluing surface, we say that fields in the image of the gluing map +are transverse to $Y$ or cuttable along $Y$. +\item There are maps $\cC_{k-1}(Y) \to \cC_k(Y \times I)$, denoted +$c \mapsto c\times I$. +These maps comprise a natural transformation of functors, and commute appropriately +with all the structure maps above (disjoint union, boundary restriction, etc.) +Furthermore, if $f: Y\times I \to Y\times I$ is a fiber-preserving homeomorphism +covering $\bar{f}:Y\to Y$, then $f(c\times I) = \bar{f}(c)\times I$. \end{enumerate} @@ -355,20 +385,20 @@ \input{text/fields.tex} + +\bigskip +\hrule +\bigskip + \nn{note: probably will suppress from notation the distinction between fields and their (orientation-reversal) duals} \nn{remark that if top dimensional fields are not already linear then we will soon linearize them(?)} -The definition of a system of fields is intended to generalize -the relevant properties of the following two examples of fields. +We now describe in more detail systems of fields coming from sub-cell-complexes labeled +by $n$-category morphisms. -The first example: Fix a target space $B$ and define $\cC(X)$ (where $X$ -is a manifold of dimension $n$ or less) to be the set of -all maps from $X$ to $B$. - -The second example will take longer to explain. Given an $n$-category $C$ with the right sort of duality (e.g. pivotal 2-category, 1-category with duals, star 1-category, disklike $n$-category), we can construct a system of fields as follows. @@ -491,14 +521,17 @@ \subsection{Local relations} \label{sec:local-relations} +\nn{the following is not done yet} + Let $B^n$ denote the standard $n$-ball. A {\it local relation} is a collection subspaces $U(B^n; c) \sub \cC_l(B^n; c)$ -(for all $c \in \cC(\bd B^n)$) satisfying the following (three?) properties. +(for all $c \in \cC(\bd B^n)$) satisfying the following two properties. +\begin{enumerate} +\item local relations imply (extended) isotopy \nn{...} +\item $U(B^n; \cdot)$ is an ideal w.r.t.\ gluing \nn{...} +\end{enumerate} +See \cite{kw:tqft} for details. -\nn{Roughly, these are (1) the local relations imply (extended) isotopy; -(2) $U(B^n; \cdot)$ is an ideal w.r.t.\ gluing; and -(3) this ideal is generated by ``small" generators (contained in an open cover of $B^n$). -See \cite{kw:tqft} for details. Need to transfer details to here.} For maps into spaces, $U(B^n; c)$ is generated by things of the form $a-b \in \cC_l(B^n; c)$, where $a$ and $b$ are maps (fields) which are homotopic rel boundary.