# HG changeset patch # User Scott Morrison # Date 1313096078 25200 # Node ID 61541264d4b3c4629447a00f777b027892a4ff43 # Parent d5caffd01b72f35ebd9703961e0b71a0443162f1 finishing most of the minor/typo issues from the referee diff -r d5caffd01b72 -r 61541264d4b3 RefereeReport.pdf Binary file RefereeReport.pdf has changed diff -r d5caffd01b72 -r 61541264d4b3 diagrams/ncat/boundary-collar.pdf Binary file diagrams/ncat/boundary-collar.pdf has changed diff -r d5caffd01b72 -r 61541264d4b3 text/basic_properties.tex --- a/text/basic_properties.tex Thu Aug 11 13:26:00 2011 -0700 +++ b/text/basic_properties.tex Thu Aug 11 13:54:38 2011 -0700 @@ -90,7 +90,7 @@ $r$ be the restriction of $b$ to $X\setminus S$. Note that $S$ is a disjoint union of balls. Assign to $b$ the acyclic (in positive degrees) subcomplex $T(b) \deq r\bullet\bc_*(S)$. -Note that if a diagram $b'$ is part of $\bd b$ then $T(B') \sub T(b)$. +Note that if a diagram $b'$ is part of $\bd b$ then $T(b') \sub T(b)$. Both $f$ and the identity are compatible with $T$ (in the sense of acyclic models, \S\ref{sec:moam}), so $f$ and the identity map are homotopic. \end{proof} diff -r d5caffd01b72 -r 61541264d4b3 text/blobdef.tex --- a/text/blobdef.tex Thu Aug 11 13:26:00 2011 -0700 +++ b/text/blobdef.tex Thu Aug 11 13:54:38 2011 -0700 @@ -156,7 +156,7 @@ \end{itemize} Combining these two operations can give rise to configurations of blobs whose complement in $X$ is not a manifold. -Thus will need to be more careful when speaking of a field $r$ on the complement of the blobs. +Thus we will need to be more careful when speaking of a field $r$ on the complement of the blobs. \begin{example} \label{sin1x-example} Consider the four subsets of $\Real^3$, @@ -208,7 +208,7 @@ %and the entire configuration should be compatible with some gluing decomposition of $X$. \begin{defn} \label{defn:configuration} -A configuration of $k$ blobs in $X$ is an ordered collection of $k$ subsets $\{B_1, \ldots B_k\}$ +A configuration of $k$ blobs in $X$ is an ordered collection of $k$ subsets $\{B_1, \ldots, B_k\}$ of $X$ such that there exists a gluing decomposition $M_0 \to \cdots \to M_m = X$ of $X$ and for each subset $B_i$ there is some $0 \leq l \leq m$ and some connected component $M_l'$ of $M_l$ which is a ball, so $B_i$ is the image of $M_l'$ in $X$. @@ -238,7 +238,7 @@ \label{defn:blob-diagram} A $k$-blob diagram on $X$ consists of \begin{itemize} -\item a configuration $\{B_1, \ldots B_k\}$ of $k$ blobs in $X$, +\item a configuration $\{B_1, \ldots, B_k\}$ of $k$ blobs in $X$, \item and a field $r \in \cF(X)$ which is splittable along some gluing decomposition compatible with that configuration, \end{itemize} such that diff -r d5caffd01b72 -r 61541264d4b3 text/evmap.tex --- a/text/evmap.tex Thu Aug 11 13:26:00 2011 -0700 +++ b/text/evmap.tex Thu Aug 11 13:54:38 2011 -0700 @@ -123,7 +123,7 @@ Let $g_j = f_1\circ f_2\circ\cdots\circ f_j$. Let $g$ be the last of the $g_j$'s. Choose the sequence $\bar{f}_j$ so that -$g(B)$ is contained is an open set of $\cV_1$ and +$g(B)$ is contained in an open set of $\cV_1$ and $g_{j-1}(|f_j|)$ is also contained in an open set of $\cV_1$. There are 1-blob diagrams $c_{ij} \in \bc_1(B)$ such that $c_{ij}$ is compatible with $\cV_1$ @@ -325,7 +325,7 @@ \end{proof} For $S\sub X$, we say that $a\in \btc_k(X)$ is {\it supported on $S$} -if there exists $a'\in \btc_k(S)$ +if there exist $a'\in \btc_k(S)$ and $r\in \btc_0(X\setmin S)$ such that $a = a'\bullet r$. \newcommand\sbtc{\btc^{\cU}} @@ -385,7 +385,7 @@ Now let $b$ be a generator of $C_2$. If $\cU$ is fine enough, there is a disjoint union of balls $V$ on which $b + h_1(\bd b)$ is supported. -Since $\bd(b + h_1(\bd b)) = s(\bd b) \in \bc_2(X)$, we can find +Since $\bd(b + h_1(\bd b)) = s(\bd b) \in \bc_1(X)$, we can find $s(b)\in \bc_2(X)$ with $\bd(s(b)) = \bd(b + h_1(\bd b))$ (by Corollary \ref{disj-union-contract}). By Lemmas \ref{bt-contract} and \ref{btc-prod}, we can now find $h_2(b) \in \btc_3(X)$, also supported on $V$, such that $\bd(h_2(b)) = s(b) - b - h_1(\bd b)$ diff -r d5caffd01b72 -r 61541264d4b3 text/hochschild.tex --- a/text/hochschild.tex Thu Aug 11 13:26:00 2011 -0700 +++ b/text/hochschild.tex Thu Aug 11 13:54:38 2011 -0700 @@ -293,7 +293,7 @@ $\widetilde{q} \in \ker(C \tensor E \tensor C \to E)$. Further, \begin{align*} -\hat{g}(\widetilde{q}) & = \sum_i \left(a_i \tensor g(\widetilde{q_i}) \tensor b_i\right) - 1 \tensor \left(\sum_i a_i g(\widetilde{q_i}\right) b_i) \tensor 1 \\ +\hat{g}(\widetilde{q}) & = \sum_i \left(a_i \tensor g(\widetilde{q_i}) \tensor b_i\right) - 1 \tensor \left(\sum_i a_i g(\widetilde{q_i}) b_i\right) \tensor 1 \\ & = q - 0 \end{align*} (here we used that $g$ is a map of $C$-$C$ bimodules, and that $\sum_i a_i q_i b_i = 0$). @@ -341,7 +341,7 @@ $j$-th term have labelled points $d_{j,i}$ to the left of $*$, $m_j$ at $*$, and $d_{j,i}'$ to the right of $*$, and there are labels $c_i$ at the labeled points outside the blob. We know that -$$\sum_j d_{j,1} \tensor \cdots \tensor d_{j,k_j} \tensor m_j \tensor d_{j,1}' \tensor \cdots \tensor d_{j,k'_j}' \in \ker(\DirectSum_{k,k'} C^{\tensor k} \tensor M \tensor C^{\tensor k'} \tensor \to M),$$ +$$\sum_j d_{j,1} \tensor \cdots \tensor d_{j,k_j} \tensor m_j \tensor d_{j,1}' \tensor \cdots \tensor d_{j,k'_j}' \in \ker(\DirectSum_{k,k'} C^{\tensor k} \tensor M \tensor C^{\tensor k'} \to M),$$ and so \begin{align*} \ev(\bdy y) & = \sum_j m_j d_{j,1}' \cdots d_{j,k'_j}' c_1 \cdots c_k d_{j,1} \cdots d_{j,k_j} \\ diff -r d5caffd01b72 -r 61541264d4b3 text/ncat.tex --- a/text/ncat.tex Thu Aug 11 13:26:00 2011 -0700 +++ b/text/ncat.tex Thu Aug 11 13:54:38 2011 -0700 @@ -984,7 +984,7 @@ There are two differences. First, for the $n$-category definition we restrict our attention to balls (and their boundaries), while for fields we consider all manifolds. -Second, in category definition we directly impose isotopy +Second, in the category definition we directly impose isotopy invariance in dimension $n$, while in the fields definition we instead remember a subspace of local relations which contain differences of isotopic fields. (Recall that the compensation for this complication is that we can demand that the gluing map for fields is injective.) @@ -1239,7 +1239,7 @@ If $X$ is an $n$-ball, we define $\cC^A(X)$ via a colimit construction. (Plain colimit, not homotopy colimit.) Let $J$ be the category whose objects are embeddings of a disjoint union of copies of -the standard ball $B^n$ into $X$, and who morphisms are given by engulfing some of the +the standard ball $B^n$ into $X$, and whose morphisms are given by engulfing some of the embedded balls into a single larger embedded ball. To each object of $J$ we associate $A^{\times m}$ (where $m$ is the number of balls), and to each morphism of $J$ we associate a morphism coming from the $\cE\cB_n$ action on $A$. @@ -1488,7 +1488,7 @@ \end{equation*} where $K$ is the vector space spanned by elements $a - g(a)$, with $a\in \psi_{\cC;W,c}(x)$ for some decomposition $x$, and $g: \psi_{\cC;W,c}(x) -\to \psi_{\cC;W,c}(y)$ is value of $\psi_{\cC;W,c}$ on some antirefinement $x \leq y$. +\to \psi_{\cC;W,c}(y)$ is the value of $\psi_{\cC;W,c}$ on some antirefinement $x \leq y$. In the $A_\infty$ case, enriched over chain complexes, the concrete description of the homotopy colimit is more involved. @@ -1576,7 +1576,7 @@ Let $z$ be a decomposition of $W$ which is in general position with respect to all of the $x_i$'s and $v_i$'s. -There there decompositions $x'_i$ and $v'_i$ (for all $i$) such that +There exist decompositions $x'_i$ and $v'_i$ (for all $i$) such that \begin{itemize} \item $x'_i$ antirefines to $x_i$ and $z$; \item $v'_i$ antirefines to $x'_i$, $x'_{i-1}$ and $v_i$; diff -r d5caffd01b72 -r 61541264d4b3 text/tqftreview.tex --- a/text/tqftreview.tex Thu Aug 11 13:26:00 2011 -0700 +++ b/text/tqftreview.tex Thu Aug 11 13:54:38 2011 -0700 @@ -393,7 +393,7 @@ These motivate the following definition. \begin{defn} -A {\it local relation} is a collection subspaces $U(B; c) \sub \lf(B; c)$, +A {\it local relation} is a collection of subspaces $U(B; c) \sub \lf(B; c)$, for all $n$-manifolds $B$ which are homeomorphic to the standard $n$-ball and all $c \in \cC(\bd B)$, satisfying the following properties.