
diff -r 8df553394931 -r 8bff31138721 text/ncat.tex
--- a/text/ncat.tex	Sun Nov 08 03:59:37 2009 +0000
+++ b/text/ncat.tex	Sun Nov 08 04:08:58 2009 +0000
@@ -309,7 +309,7 @@
 \end{eqnarray*}
 (See Figure \ref{glue-collar}.)
 \begin{figure}[!ht]\begin{equation*}
-\mathfig{.9}{tempkw/glue-collar}
+\mathfig{.9}{tempkw/blah10}
 \end{equation*}\caption{Extended homeomorphism.}\label{glue-collar}\end{figure}
 We say that $\psi_{Y,J}$ is {\it extended isotopic} to the identity map.
 \nn{bad terminology; fix it later}
@@ -617,6 +617,10 @@
 (If $\cD$ were a general TQFT, we would define $\cM(B, N)$ to be
 the subset of $\cD((B\times \bd W)\cup (N\times W))$ which is splittable along $N\times \bd W$.)
 
+\begin{figure}[!ht]
+$$\mathfig{.8}{tempkw/blah15}$$
+\caption{From manifold with boundary collar to marked ball}\label{blah15}\end{figure}
+
 Define the boundary of a marked $k$-ball $(B, N)$ to be the pair $(\bd B \setmin N, \bd N)$.
 Call such a thing a {marked $k{-}1$-hemisphere}.
 




