aomart (12apr21)

git-svn-id: svn://tug.org/texlive/trunk@58855 c570f23f-e606-0410-a88d-b1316a301751

10 files changed, 77 insertions, 43 deletions

diff --git a/Master/texmf-dist/doc/latex/aomart/README b/Master/texmf-dist/doc/latex/aomart/README
index 31738d4abed..2fa8715ea8d 100644
--- a/Master/texmf-dist/doc/latex/aomart/README
+++ b/Master/texmf-dist/doc/latex/aomart/README
@@ -1,12 +1,15 @@
 	      LaTeX Class for The Annals of Mathematics
 			    Boris Veytsman
-			    Version 1.24
+			    Version 1.25
 
 This package provides the class for typesetting articles for The Annals
 of Mathematics, http://annals.princeton.edu/.  
 
 Changes:
 
+    Version 1.25
+          New command: \fullpageref
+
     Version 1.24
           Optionally print MSC designation
 
diff --git a/Master/texmf-dist/doc/latex/aomart/aomart.pdf b/Master/texmf-dist/doc/latex/aomart/aomart.pdf
index 58366ab2604..1ae47991e84 100644
--- a/Master/texmf-dist/doc/latex/aomart/aomart.pdf
+++ b/Master/texmf-dist/doc/latex/aomart/aomart.pdf
diff --git a/Master/texmf-dist/doc/latex/aomart/aomfrench.pdf b/Master/texmf-dist/doc/latex/aomart/aomfrench.pdf
index 5b411b76b1b..2412c929015 100644
--- a/Master/texmf-dist/doc/latex/aomart/aomfrench.pdf
+++ b/Master/texmf-dist/doc/latex/aomart/aomfrench.pdf
diff --git a/Master/texmf-dist/doc/latex/aomart/aomsample.pdf b/Master/texmf-dist/doc/latex/aomart/aomsample.pdf
index 817a42f5ee9..1faf78a4e94 100644
--- a/Master/texmf-dist/doc/latex/aomart/aomsample.pdf
+++ b/Master/texmf-dist/doc/latex/aomart/aomsample.pdf
diff --git a/Master/texmf-dist/doc/latex/aomart/aomsample.tex b/Master/texmf-dist/doc/latex/aomart/aomsample.tex
index 9d331b0b85e..2ecba3e18d7 100644
--- a/Master/texmf-dist/doc/latex/aomart/aomsample.tex
+++ b/Master/texmf-dist/doc/latex/aomart/aomsample.tex
@@ -365,7 +365,7 @@ D(t_1,\dots,t_n)
 where $\mathbf{K}(t=1,t_1,\dots,t_n; i|i)$ is the $i$th principal
 submatrix of $\mathbf{K}(t=1,t_1,\dots,t_n)$.
 
-Theorem ~\ref{thm-main} leads to
+Theorem~\ref{thm-main} leads to
 \begin{equation}\label{detK1}
 \det\mathbf{K}(t_1,t_1,\dots,t_n)
 =\sum_{I\in\mathbf{n}}(-1)^{\envert{I}}t^{n-\envert{I}}
@@ -379,7 +379,7 @@ Note that
 ^{(\lambda)}(\overline{I}|\overline{I})=0.
 \end{equation}
 
-Let $t_i=\hat x_i,i=1,\dots,n$. Lemma ~\ref{lem-per} yields
+Let $t_i=\hat x_i,i=1,\dots,n$. Lemma~\ref{lem-per} yields
 \begin{multline}
 \biggl(\sum_{\,i\in\mathbf{n}}a_{l _i}x_i\biggr)
 \det\mathbf{K}(t=1,x_1,\dots,x_n;l |l )\\
@@ -421,8 +421,8 @@ D(t_1,\dots,t_n)}_{t_i=\left\{\begin{smallmatrix}
 \section{Application}
 \label{lincomp}
 
-We consider here the applications of Theorems~\ref{th-info-ow-ow} and
-~\ref{th-weak-ske-owf} to a complete
+We consider here the applications of Theorems~\ref{th-info-ow-ow}
+and~\ref{th-weak-ske-owf} on page~\pageref{th-weak-ske-owf} to a complete
 multipartite graph $K_{n_1\dots n_p}$. It can be shown that the
 number of spanning trees of $K_{n_1\dots n_p}$
 may be written
@@ -463,7 +463,7 @@ H_c&=\frac12\sum^{n-1}_{l =0}
 \end{equation}
 
 The enumeration of $H_c$ in a $K_{n_1\dotsm n_p}$ graph can also be
-carried out by Theorem ~\ref{thm-H-param} or ~\ref{thm-asym}
+carried out by Theorem~\ref{thm-H-param} or~\ref{thm-asym}
 together with the algebraic method of \eqref{multdef}.
 Some elegant representations may be obtained. For example, $H_c$ in
 a $K_{n_1n_2n_3}$ graph may be written
@@ -930,8 +930,8 @@ achieve the general result using \thmref{t:conl}.
 
 \begin{step}
 Assume that $n=1$. Since $S_u$ is at most countable, \eqref{sum-bij}
-yields that $\abs{\wt{D}v}(S_u\backslash S_v)=0$, so that
-\eqref{e:st} and \eqref{e:barwq} imply that $Dv=\wt{D}v+Jv$ is
+yields that $\abs{\wt{D}v}(S_u\backslash S_v)=0$, so that~\eqref{e:st}
+and \eqref{e:barwq} imply that $Dv=\wt{D}v+Jv$ is 
 the Radon-Nikod\'ym decomposition of $Dv$ in absolutely continuous and
 singular part with respect to $\abs{\wt{D} u}$. By
 \thmref{th-weak-ske-owf}, we have
@@ -959,8 +959,8 @@ and
 \hat v(t)=f(\hat u(t))\qquad\forall t\in\mathbf{R}.\end{equation}
 Let $t\in\mathbf{R}$ be such that
 $\abs{\wt{D}u}(\interval{\left[t,s\right[})>0$ for every $s>t$ and
-assume that the limits in \eqref{joe} exist. By \eqref{j:mark} and
-\eqref{far-d} we get
+assume that the limits in \eqref{joe} exist. By \eqref{j:mark}
+and~\eqref{far-d} we get 
 \begin{equation*}\begin{split}
 \frac{\hat v(s)-\hat
 v(t)}{\abs{\wt{D}u}(\interval{\left[t,s\right[})}&=\frac {f(\hat
@@ -1021,8 +1021,8 @@ for $\mathcal{H}_{n-1}$-almost every $y\in \pi_\nu$. We claim that
 }}(y+t\nu)=\frac{\wt{D}u_y}
 {\abs{\wt{D}u_y}}(t)\qquad\abs{\wt{D}u_y}\text{-a.e. in }\mathbf{R}
 \end{equation}
-for $\mathcal{H}_{n-1}$-almost every $y\in\pi_\nu$. In fact, by
-\eqref{sum-ali} and \eqref{delta-l} we get
+for $\mathcal{H}_{n-1}$-almost every $y\in\pi_\nu$. In fact,
+by~\eqref{sum-ali} and \eqref{delta-l} we get
 \begin{multline*}
 \int_{\pi_\nu}\frac{\wt{D}u_y}{\abs{\wt{D}u_y}}\cdot\abs{\wt{D}u_y
 }\,d\mathcal{H}_{n-1}(y)=\int_{\pi_\nu}\wt{D}u_y\,d\mathcal{H}_{n-1}(y)\\
@@ -1046,8 +1046,7 @@ u,\nu\rangle }{\abs{\langle \wt{D}u,\nu\rangle }}(y+t\nu))-f(\tilde
 u(y+t\nu))}{h}
 =\frac{\langle \wt{D}v,\nu\rangle }{\abs{\langle
 \wt{D}u,\nu\rangle }}(y+t\nu)\]
-for $\mathcal{H}_{n-1}$-almost every $y\in\pi_\nu$, and using again
-\eqref{detK1}, \eqref{detK2} we get
+for $\mathcal{H}_{n-1}$-almost every $y\in\pi_\nu$, and using again~\eqref{detK1}, \eqref{detK2} we get
 \[
 \lim_{h\to 0}\frac{f(\tilde u(x)+h\dfrac{\langle
 \wt{D}u,\nu\rangle }{\abs{\langle \wt{D}u,\nu\rangle }}(x))-f(\tilde
@@ -1126,8 +1125,9 @@ A^{(\lambda)}_l =\sum_{I_l \subseteq\mathbf{n}}\per \mathbf{A}
 \end{thm}
 
 It is worth noting that $A_l ^{(\lambda)}$ of \eqref{A-l-lambda} is
-similar to the coefficients $b_l $ of the characteristic polynomial of
-\eqref{bl-sum}. It is well known in graph theory that the coefficients
+similar to the coefficients $b_l $ of the characteristic polynomial
+of~\eqref{bl-sum}. It is well known in graph theory that the
+coefficients 
 $b_l $ can be expressed as a sum over certain subgraphs. It is
 interesting to see whether $A_l $, $\lambda=0$, structural properties
 of a graph.
@@ -1153,7 +1153,7 @@ A_l =
 0,&\text{otherwise }.\end{cases}
 \label{compl-bip-gr}
 \end{equation}
-Theorem ~\ref{thm-H-param}
+Theorem~\ref{thm-H-param}
 leads to
 \begin{equation}
 H_c=\frac1{n_1+n_2}n_1!n_2!\delta_{n_1n_2}.
diff --git a/Master/texmf-dist/doc/latex/aomart/aomsample1.pdf b/Master/texmf-dist/doc/latex/aomart/aomsample1.pdf
index cbc4470d341..da11f5c5743 100644
--- a/Master/texmf-dist/doc/latex/aomart/aomsample1.pdf
+++ b/Master/texmf-dist/doc/latex/aomart/aomsample1.pdf
diff --git a/Master/texmf-dist/doc/latex/aomart/aomsample1.tex b/Master/texmf-dist/doc/latex/aomart/aomsample1.tex
index 29257baeadd..30a52e5691f 100644
--- a/Master/texmf-dist/doc/latex/aomart/aomsample1.tex
+++ b/Master/texmf-dist/doc/latex/aomart/aomsample1.tex
@@ -421,7 +421,8 @@ D(t_1,\dots,t_n)}_{t_i=\left\{\begin{smallmatrix}
 \section{Application}
 \label{lincomp}
 
-We consider here the applications of \fullref{Theorems}{th-info-ow-ow} \fullref{and}{th-weak-ske-owf} to a complete
+We consider here the applications of \fullref{Theorems}{th-info-ow-ow}
+\fullref{and}{th-weak-ske-owf} on \fullpageref[page]{th-weak-ske-owf} to a complete
 multipartite graph $K_{n_1\dots n_p}$. It can be shown that the
 number of spanning trees of $K_{n_1\dots n_p}$
 may be written
@@ -928,7 +929,8 @@ achieve the general result using \thmref{t:conl}.
 
 \begin{step}
 Assume that $n=1$. Since $S_u$ is at most countable, \eqref{sum-bij}
-yields that $\abs{\wt{D}v}(S_u\backslash S_v)=0$, so that \eqref{e:st} and \eqref{e:barwq} imply that $Dv=\wt{D}v+Jv$ is
+yields that $\abs{\wt{D}v}(S_u\backslash S_v)=0$, so that~\eqref{e:st}
+and \eqref{e:barwq} imply that $Dv=\wt{D}v+Jv$ is 
 the Radon-Nikod\'ym decomposition of $Dv$ in absolutely continuous and
 singular part with respect to $\abs{\wt{D} u}$. By
 \thmref{th-weak-ske-owf}, we have
@@ -956,7 +958,8 @@ and
 \hat v(t)=f(\hat u(t))\qquad\forall t\in\mathbf{R}.\end{equation}
 Let $t\in\mathbf{R}$ be such that
 $\abs{\wt{D}u}(\interval{\left[t,s\right[})>0$ for every $s>t$ and
-assume that the limits in \eqref{joe} exist. By \eqref{j:mark} and \eqref{far-d} we get
+assume that the limits in \eqref{joe} exist. By \eqref{j:mark}
+and~\eqref{far-d} we get 
 \begin{equation*}\begin{split}
 \frac{\hat v(s)-\hat
 v(t)}{\abs{\wt{D}u}(\interval{\left[t,s\right[})}&=\frac {f(\hat
@@ -1017,7 +1020,8 @@ for $\mathcal{H}_{n-1}$-almost every $y\in \pi_\nu$. We claim that
 }}(y+t\nu)=\frac{\wt{D}u_y}
 {\abs{\wt{D}u_y}}(t)\qquad\abs{\wt{D}u_y}\text{-a.e. in }\mathbf{R}
 \end{equation}
-for $\mathcal{H}_{n-1}$-almost every $y\in\pi_\nu$. In fact, by \eqref{sum-ali} and \eqref{delta-l} we get
+for $\mathcal{H}_{n-1}$-almost every $y\in\pi_\nu$. In fact,
+by~\eqref{sum-ali} and \eqref{delta-l} we get
 \begin{multline*}
 \int_{\pi_\nu}\frac{\wt{D}u_y}{\abs{\wt{D}u_y}}\cdot\abs{\wt{D}u_y
 }\,d\mathcal{H}_{n-1}(y)=\int_{\pi_\nu}\wt{D}u_y\,d\mathcal{H}_{n-1}(y)\\
@@ -1041,7 +1045,7 @@ u,\nu\rangle }{\abs{\langle \wt{D}u,\nu\rangle }}(y+t\nu))-f(\tilde
 u(y+t\nu))}{h}
 =\frac{\langle \wt{D}v,\nu\rangle }{\abs{\langle
 \wt{D}u,\nu\rangle }}(y+t\nu)\]
-for $\mathcal{H}_{n-1}$-almost every $y\in\pi_\nu$, and using again \eqref{detK1}, \eqref{detK2} we get
+for $\mathcal{H}_{n-1}$-almost every $y\in\pi_\nu$, and using again~\eqref{detK1}, \eqref{detK2} we get
 \[
 \lim_{h\to 0}\frac{f(\tilde u(x)+h\dfrac{\langle
 \wt{D}u,\nu\rangle }{\abs{\langle \wt{D}u,\nu\rangle }}(x))-f(\tilde
@@ -1120,7 +1124,9 @@ A^{(\lambda)}_l =\sum_{I_l \subseteq\mathbf{n}}\per \mathbf{A}
 \end{thm}
 
 It is worth noting that $A_l ^{(\lambda)}$ of \eqref{A-l-lambda} is
-similar to the coefficients $b_l $ of the characteristic polynomial of \eqref{bl-sum}. It is well known in graph theory that the coefficients
+similar to the coefficients $b_l $ of the characteristic polynomial
+of~\eqref{bl-sum}. It is well known in graph theory that the
+coefficients 
 $b_l $ can be expressed as a sum over certain subgraphs. It is
 interesting to see whether $A_l $, $\lambda=0$, structural properties
 of a graph.
diff --git a/Master/texmf-dist/doc/latex/aomart/fullref.pl b/Master/texmf-dist/doc/latex/aomart/fullref.pl
index 0414089ea00..0eba808aa84 100644
--- a/Master/texmf-dist/doc/latex/aomart/fullref.pl
+++ b/Master/texmf-dist/doc/latex/aomart/fullref.pl
@@ -4,7 +4,7 @@
 # perl fullref.pl original.tex > converted.tex
 #
 #
-# Copyright (C) 2010 Annals of Mathematics.  Public domain.
+# Copyright (C) 2010-2021 Annals of Mathematics.  Licenses under CC0
 #
 # Author: Boris Veytsman
 #
@@ -44,7 +44,7 @@ while (<>) {
     }
     s/(\s)([^\s\\]\S*[^~\s\(\)\[\]])[\s~]*\[\\ref\{([^\}]+)\}\]/$1\\bfullref{$2}{$3}/g;
     s/(\s)([^\s\\]\S*[^~\s\(\)\[\]])[\s~]*\\ref\{([^\}]+)\}/$1\\fullref{$2}{$3}/g;
-
+    s/(\s)([^\s\\]\S*[^~\s\(\)\[\]])[\s~]*\\pageref\{([^\}]+)\}/$1\\fullpageref[$2]{$3}/g;
     # Now delete the extra space
     s/^ //;
     $prevline=$_;
diff --git a/Master/texmf-dist/source/latex/aomart/aomart.dtx b/Master/texmf-dist/source/latex/aomart/aomart.dtx
index 3bfbf3390ab..f5e7e0d0252 100644
--- a/Master/texmf-dist/source/latex/aomart/aomart.dtx
+++ b/Master/texmf-dist/source/latex/aomart/aomart.dtx
@@ -1,7 +1,7 @@
 % \iffalse
-% $Id: aomart.dtx,v 1.77 2020/08/09 22:26:46 boris Exp $
+% $Id: aomart.dtx,v 1.78 2021/04/11 00:14:37 boris Exp $
 %
-% Copyright 2010-2020, Princeton University (Mathematics Department)
+% Copyright 2010-2021, Princeton University (Mathematics Department)
 % This work may be distributed and/or modified under the
 % conditions of the LaTeX Project Public License, either
 % version 1.3 of this license or (at your option) any 
@@ -23,7 +23,7 @@
 % public domain.
 %
 % \fi 
-% \CheckSum{1532}
+% \CheckSum{1536}
 %
 %
 %% \CharacterTable
@@ -66,7 +66,7 @@
 % \GetFileInfo{aomart.dtx}
 % \newcommand{\progname}[1]{\textsf{#1}}
 % \title{\LaTeX{} Class for The \emph{Annals of
-% Mathematics}\thanks{\copyright 2010--2020, Princeton University
+% Mathematics}\thanks{\copyright 2010--2021, Princeton University
 % (Mathematics Department)}} 
 % \author{Boris Veytsman\thanks{%
 % \href{mailto:borisv@lk.net}{\texttt{borisv@lk.net}},
@@ -574,10 +574,11 @@
 % \end{verbatim}
 %
 %
-% \DescribeMacro{\fullref}
-% \DescribeMacro{\pfullref}
-% \DescribeMacro{\bfullref}
-% \DescribeMacro{\eqfullref}
+% \DescribeMacro{\fullref}%
+% \DescribeMacro{\pfullref}%
+% \DescribeMacro{\bfullref}%
+% \DescribeMacro{\eqfullref}%
+% \DescribeMacro{\fullpageref}%
 % A set of macros is used to make more convenient clickable references
 % in the online versions of papers.  The
 % package~\progname{hyperref}~\cite{Rahtz06:Hyperref} 
@@ -600,6 +601,19 @@
 % \begin{verbatim}
 % ...see \eqfullref{equation}{eq:alpha}...
 % \end{verbatim}
+% The similar command  |\fullpageref| is used to make the word
+% ``page'' clickable, for example,
+% \begin{verbatim}
+% ...see \eqfullref{equation}{eq:alpha} on
+% \fullpageref{eq:alpha}...
+% \end{verbatim}
+% By default the command adds the word ``page'' to the text.  You can
+% override this choice using the optiomal parameter, e.g.
+% \begin{verbatim}
+% \fullpageref[The page]{eq:alpha} starts the discussion of...
+% \end{verbatim}
+% 
+%
 %
 % The \progname{Perl} script \path{fullref.pl} can be used to convert
 % change all references to the |\fullref| commands.  It works in the
@@ -607,14 +621,15 @@
 % \begin{verbatim}
 % perl fullref.pl original.pl > result.pl
 % \end{verbatim}
-% The script converts all instances of combinations ``|word \ref{reference}|''
-% and ``|word~\ref{reference}|''
-% to ``|\fullref{word}{reference}|, and similarly for
-% parenthesized references or |\eqref| commands.  To prevent the
-% converting, just put |\ref{reference}| or |\eqref{reference}| inside
-% braces.  The ``word'' here must not start with a backslash
-% (i.e. must not be a macro itself).  This prevents disastrous results
-% for phrases like ``|see~\ref{a}, \ref{b}|''.
+% The script converts all instances of combinations
+% ``|word \ref{reference}|'', ``|word~\ref{reference}|'' and
+% ``|word~\pageref{reference}|'' to ``|\fullref{word}{reference}|, and
+% similarly for parenthesized references, |\eqref| commands, and page
+% references.  To prevent the converting, just put |\ref{reference}|
+% or |\eqref{reference}| inside braces.  The ``word'' here must not
+% start with a backslash (i.e. must not be a macro itself).  This
+% prevents disastrous results for phrases like
+% ``|see~\ref{a},  \ref{b}|''.
 %
 %
 % The distribution includes two sample files, \path{aomsample.tex} and
@@ -781,7 +796,7 @@
 \ProvidesFile{aomart.dtx}
 %</gobble>
 %<class>\ProvidesClass{aomart}
-[2020/08/09 v1.24 Typesetting articles for the Annals of Mathematics]
+[2021/04/10 v1.25 Typesetting articles for the Annals of Mathematics]
 %    \end{macrocode}
 %
 %
@@ -2322,6 +2337,15 @@
 \newcommand{\eqfullref}[2]{\hyperref[#2]{#1~\textup{\tagform@{\ref*{#2}}}}}
 %    \end{macrocode}   
 % \end{macro}
+% \begin{macro}{\fullpageref}
+% \changes{v1.25}{2021/04/10}{Added macro} 
+%   A wide link for page reference.  Note that the word ``page'' can
+%   be omitted
+%    \begin{macrocode}
+\newcommand{\fullpageref}[2][page]{\hyperref[#2]{#1~\pageref*{#2}}}
+%    \end{macrocode}
+% \end{macro}
+%
 %
 % \begin{macro}{\eqnarray}
 % \changes{v0.9}{2010/12/04}{Redefined standard macro} 
diff --git a/Master/texmf-dist/tex/latex/aomart/aomart.cls b/Master/texmf-dist/tex/latex/aomart/aomart.cls
index 82430d1c322..539c9413def 100644
--- a/Master/texmf-dist/tex/latex/aomart/aomart.cls
+++ b/Master/texmf-dist/tex/latex/aomart/aomart.cls
@@ -37,7 +37,7 @@
 %%   Right brace   \}     Tilde         \~}
 \NeedsTeXFormat{LaTeX2e}
 \ProvidesClass{aomart}
-[2020/08/09 v1.24 Typesetting articles for the Annals of Mathematics]
+[2021/04/10 v1.25 Typesetting articles for the Annals of Mathematics]
 \long\def\aom@size@warning#1{%
   \ClassWarning{aomart}{Size-changing option #1 will not be
     honored}}%
@@ -610,6 +610,7 @@
 \newcommand{\pfullref}[2]{\@fullref{#1}{(}{#2}{)}}
 \newcommand{\bfullref}[2]{\@fullref{#1}{[}{#2}{]}}
 \newcommand{\eqfullref}[2]{\hyperref[#2]{#1~\textup{\tagform@{\ref*{#2}}}}}
+\newcommand{\fullpageref}[2][page]{\hyperref[#2]{#1~\pageref*{#2}}}
 \def\eqnarray{%
    \stepcounter{equation}%
    \def\@currentlabel{\p@equation\theequation}%