diff options
author | Karl Berry <karl@freefriends.org> | 2009-05-26 23:22:36 +0000 |
---|---|---|
committer | Karl Berry <karl@freefriends.org> | 2009-05-26 23:22:36 +0000 |
commit | 788463b73b8e87304fa052fe0f9fe43fc2217a3a (patch) | |
tree | d6612e5b5237b81281b06a6be039df71695119c4 /Master/texmf-dist/source/latex/hyperref/test | |
parent | 2be0d9eaabb3f79a9a41cb82da8e05d538f20c17 (diff) |
hyperref update (26may09)
git-svn-id: svn://tug.org/texlive/trunk@13484 c570f23f-e606-0410-a88d-b1316a301751
Diffstat (limited to 'Master/texmf-dist/source/latex/hyperref/test')
32 files changed, 5259 insertions, 0 deletions
diff --git a/Master/texmf-dist/source/latex/hyperref/test/Makefile b/Master/texmf-dist/source/latex/hyperref/test/Makefile new file mode 100644 index 00000000000..ac6fc6cb9b3 --- /dev/null +++ b/Master/texmf-dist/source/latex/hyperref/test/Makefile @@ -0,0 +1,7 @@ +all: + pdflatex test7 + pdflatex test7 + (for i in test*.tex; do pdflatex $$i;pdflatex $$i; done) + +clean: + -$(RM) test*pdf *.aux *.log *.toc *.lof *.lot *.idx *.ind *.out diff --git a/Master/texmf-dist/source/latex/hyperref/test/bit.tex b/Master/texmf-dist/source/latex/hyperref/test/bit.tex new file mode 100644 index 00000000000..9e5b4fedbaf --- /dev/null +++ b/Master/texmf-dist/source/latex/hyperref/test/bit.tex @@ -0,0 +1,2 @@ +sssssssss +\newpage diff --git a/Master/texmf-dist/source/latex/hyperref/test/hog.eps b/Master/texmf-dist/source/latex/hyperref/test/hog.eps new file mode 100644 index 00000000000..7e685f8b489 --- /dev/null +++ b/Master/texmf-dist/source/latex/hyperref/test/hog.eps @@ -0,0 +1,463 @@ +%!PS-Adobe-2.0 EPSF-2.0 +%%Title: h.eps +%%Creator: fig2dev Version 3.2 Patchlevel 1a +%%CreationDate: Mon Jul 19 12:28:51 1999 +%%For: rahtz@spqr (Sebastian Rahtz,,,) +%%Orientation: Portrait +%%BoundingBox: 0 0 251 213 +%%Pages: 0 +%%BeginSetup +%%EndSetup +%%Magnification: 1.0000 +%%EndComments +/MyAppDict 100 dict dup begin def +/$F2psDict 200 dict def +$F2psDict begin +$F2psDict /mtrx matrix put +/col-1 {0 setgray} bind def +/col0 {0.000 0.000 0.000 srgb} bind def +/col1 {0.000 0.000 1.000 srgb} bind def +/col2 {0.000 1.000 0.000 srgb} bind def +/col3 {0.000 1.000 1.000 srgb} bind def +/col4 {1.000 0.000 0.000 srgb} bind def +/col5 {1.000 0.000 1.000 srgb} bind def +/col6 {1.000 1.000 0.000 srgb} bind def +/col7 {1.000 1.000 1.000 srgb} bind def +/col8 {0.000 0.000 0.560 srgb} bind def +/col9 {0.000 0.000 0.690 srgb} bind def +/col10 {0.000 0.000 0.820 srgb} bind def +/col11 {0.530 0.810 1.000 srgb} bind def +/col12 {0.000 0.560 0.000 srgb} bind def +/col13 {0.000 0.690 0.000 srgb} bind def +/col14 {0.000 0.820 0.000 srgb} bind def +/col15 {0.000 0.560 0.560 srgb} bind def +/col16 {0.000 0.690 0.690 srgb} bind def +/col17 {0.000 0.820 0.820 srgb} bind def +/col18 {0.560 0.000 0.000 srgb} bind def +/col19 {0.690 0.000 0.000 srgb} bind def +/col20 {0.820 0.000 0.000 srgb} bind def +/col21 {0.560 0.000 0.560 srgb} bind def +/col22 {0.690 0.000 0.690 srgb} bind def +/col23 {0.820 0.000 0.820 srgb} bind def +/col24 {0.500 0.190 0.000 srgb} bind def +/col25 {0.630 0.250 0.000 srgb} bind def +/col26 {0.750 0.380 0.000 srgb} bind def +/col27 {1.000 0.500 0.500 srgb} bind def +/col28 {1.000 0.630 0.630 srgb} bind def +/col29 {1.000 0.750 0.750 srgb} bind def +/col30 {1.000 0.880 0.880 srgb} bind def +/col31 {1.000 0.840 0.000 srgb} bind def + +end +save +-191.0 342.0 translate +1 -1 scale +.9 .9 scale % to make patterns same scale as in xfig + +% This junk string is used by the show operators +/PATsstr 1 string def +/PATawidthshow { % cx cy cchar rx ry string + % Loop over each character in the string + { % cx cy cchar rx ry char + % Show the character + dup % cx cy cchar rx ry char char + PATsstr dup 0 4 -1 roll put % cx cy cchar rx ry char (char) + false charpath % cx cy cchar rx ry char + /clip load PATdraw + % Move past the character (charpath modified the + % current point) + currentpoint % cx cy cchar rx ry char x y + newpath + moveto % cx cy cchar rx ry char + % Reposition by cx,cy if the character in the string is cchar + 3 index eq { % cx cy cchar rx ry + 4 index 4 index rmoveto + } if + % Reposition all characters by rx ry + 2 copy rmoveto % cx cy cchar rx ry + } forall + pop pop pop pop pop % - + currentpoint + newpath + moveto +} bind def +/PATcg { + 7 dict dup begin + /lw currentlinewidth def + /lc currentlinecap def + /lj currentlinejoin def + /ml currentmiterlimit def + /ds [ currentdash ] def + /cc [ currentrgbcolor ] def + /cm matrix currentmatrix def + end +} bind def +% PATdraw - calculates the boundaries of the object and +% fills it with the current pattern +/PATdraw { % proc + save exch + PATpcalc % proc nw nh px py + 5 -1 roll exec % nw nh px py + newpath + PATfill % - + restore +} bind def +% PATfill - performs the tiling for the shape +/PATfill { % nw nh px py PATfill - + PATDict /CurrentPattern get dup begin + setfont + % Set the coordinate system to Pattern Space + PatternGState PATsg + % Set the color for uncolored pattezns + PaintType 2 eq { PATDict /PColor get PATsc } if + % Create the string for showing + 3 index string % nw nh px py str + % Loop for each of the pattern sources + 0 1 Multi 1 sub { % nw nh px py str source + % Move to the starting location + 3 index 3 index % nw nh px py str source px py + moveto % nw nh px py str source + % For multiple sources, set the appropriate color + Multi 1 ne { dup PC exch get PATsc } if + % Set the appropriate string for the source + 0 1 7 index 1 sub { 2 index exch 2 index put } for pop + % Loop over the number of vertical cells + 3 index % nw nh px py str nh + { % nw nh px py str + currentpoint % nw nh px py str cx cy + 2 index show % nw nh px py str cx cy + YStep add moveto % nw nh px py str + } repeat % nw nh px py str + } for + 5 { pop } repeat + end +} bind def + +% PATkshow - kshow with the current pattezn +/PATkshow { % proc string + exch bind % string proc + 1 index 0 get % string proc char + % Loop over all but the last character in the string + 0 1 4 index length 2 sub { + % string proc char idx + % Find the n+1th character in the string + 3 index exch 1 add get % string proe char char+1 + exch 2 copy % strinq proc char+1 char char+1 char + % Now show the nth character + PATsstr dup 0 4 -1 roll put % string proc chr+1 chr chr+1 (chr) + false charpath % string proc char+1 char char+1 + /clip load PATdraw + % Move past the character (charpath modified the current point) + currentpoint newpath moveto + % Execute the user proc (should consume char and char+1) + mark 3 1 roll % string proc char+1 mark char char+1 + 4 index exec % string proc char+1 mark... + cleartomark % string proc char+1 + } for + % Now display the last character + PATsstr dup 0 4 -1 roll put % string proc (char+1) + false charpath % string proc + /clip load PATdraw + neewath + pop pop % - +} bind def +% PATmp - the makepattern equivalent +/PATmp { % patdict patmtx PATmp patinstance + exch dup length 7 add % We will add 6 new entries plus 1 FID + dict copy % Create a new dictionary + begin + % Matrix to install when painting the pattern + TilingType PATtcalc + /PatternGState PATcg def + PatternGState /cm 3 -1 roll put + % Check for multi pattern sources (Level 1 fast color patterns) + currentdict /Multi known not { /Multi 1 def } if + % Font dictionary definitions + /FontType 3 def + % Create a dummy encoding vector + /Encoding 256 array def + 3 string 0 1 255 { + Encoding exch dup 3 index cvs cvn put } for pop + /FontMatrix matrix def + /FontBBox BBox def + /BuildChar { + mark 3 1 roll % mark dict char + exch begin + Multi 1 ne {PaintData exch get}{pop} ifelse % mark [paintdata] + PaintType 2 eq Multi 1 ne or + { XStep 0 FontBBox aload pop setcachedevice } + { XStep 0 setcharwidth } ifelse + currentdict % mark [paintdata] dict + /PaintProc load % mark [paintdata] dict paintproc + end + gsave + false PATredef exec true PATredef + grestore + cleartomark % - + } bind def + currentdict + end % newdict + /foo exch % /foo newlict + definefont % newfont +} bind def +% PATpcalc - calculates the starting point and width/height +% of the tile fill for the shape +/PATpcalc { % - PATpcalc nw nh px py + PATDict /CurrentPattern get begin + gsave + % Set up the coordinate system to Pattern Space + % and lock down pattern + PatternGState /cm get setmatrix + BBox aload pop pop pop translate + % Determine the bounding box of the shape + pathbbox % llx lly urx ury + grestore + % Determine (nw, nh) the # of cells to paint width and height + PatHeight div ceiling % llx lly urx qh + 4 1 roll % qh llx lly urx + PatWidth div ceiling % qh llx lly qw + 4 1 roll % qw qh llx lly + PatHeight div floor % qw qh llx ph + 4 1 roll % ph qw qh llx + PatWidth div floor % ph qw qh pw + 4 1 roll % pw ph qw qh + 2 index sub cvi abs % pw ph qs qh-ph + exch 3 index sub cvi abs exch % pw ph nw=qw-pw nh=qh-ph + % Determine the starting point of the pattern fill + %(px, py) + 4 2 roll % nw nh pw ph + PatHeight mul % nw nh pw py + exch % nw nh py pw + PatWidth mul exch % nw nh px py + end +} bind def + +% Save the original routines so that we can use them later on +/oldfill /fill load def +/oldeofill /eofill load def +/oldstroke /stroke load def +/oldshow /show load def +/oldashow /ashow load def +/oldwidthshow /widthshow load def +/oldawidthshow /awidthshow load def +/oldkshow /kshow load def + +% These defs are necessary so that subsequent procs don't bind in +% the originals +/fill { oldfill } bind def +/eofill { oldeofill } bind def +/stroke { oldstroke } bind def +/show { oldshow } bind def +/ashow { oldashow } bind def +/widthshow { oldwidthshow } bind def +/awidthshow { oldawidthshow } bind def +/kshow { oldkshow } bind def +/PATredef { + MyAppDict begin + { + /fill { /clip load PATdraw newpath } bind def + /eofill { /eoclip load PATdraw newpath } bind def + /stroke { PATstroke } bind def + /show { 0 0 null 0 0 6 -1 roll PATawidthshow } bind def + /ashow { 0 0 null 6 3 roll PATawidthshow } + bind def + /widthshow { 0 0 3 -1 roll PATawidthshow } + bind def + /awidthshow { PATawidthshow } bind def + /kshow { PATkshow } bind def + } { + /fill { oldfill } bind def + /eofill { oldeofill } bind def + /stroke { oldstroke } bind def + /show { oldshow } bind def + /ashow { oldashow } bind def + /widthshow { oldwidthshow } bind def + /awidthshow { oldawidthshow } bind def + /kshow { oldkshow } bind def + } ifelse + end +} bind def +false PATredef +% Conditionally define setcmykcolor if not available +/setcmykcolor where { pop } { + /setcmykcolor { + 1 sub 4 1 roll + 3 { + 3 index add neg dup 0 lt { pop 0 } if 3 1 roll + } repeat + setrgbcolor - pop + } bind def +} ifelse +/PATsc { % colorarray + aload length % c1 ... cn length + dup 1 eq { pop setgray } { 3 eq { setrgbcolor } { setcmykcolor + } ifelse } ifelse +} bind def +/PATsg { % dict + begin + lw setlinewidth + lc setlinecap + lj setlinejoin + ml setmiterlimit + ds aload pop setdash + cc aload pop setrgbcolor + cm setmatrix + end +} bind def + +/PATDict 3 dict def +/PATsp { + true PATredef + PATDict begin + /CurrentPattern exch def + % If it's an uncolored pattern, save the color + CurrentPattern /PaintType get 2 eq { + /PColor exch def + } if + /CColor [ currentrgbcolor ] def + end +} bind def +% PATstroke - stroke with the current pattern +/PATstroke { + countdictstack + save + mark + { + currentpoint strokepath moveto + PATpcalc % proc nw nh px py + clip newpath PATfill + } stopped { + (*** PATstroke Warning: Path is too complex, stroking + with gray) = + cleartomark + restore + countdictstack exch sub dup 0 gt + { { end } repeat } { pop } ifelse + gsave 0.5 setgray oldstroke grestore + } { pop restore pop } ifelse + newpath +} bind def +/PATtcalc { % modmtx tilingtype PATtcalc tilematrix + % Note: tiling types 2 and 3 are not supported + gsave + exch concat % tilingtype + matrix currentmatrix exch % cmtx tilingtype + % Tiling type 1 and 3: constant spacing + 2 ne { + % Distort the pattern so that it occupies + % an integral number of device pixels + dup 4 get exch dup 5 get exch % tx ty cmtx + XStep 0 dtransform + round exch round exch % tx ty cmtx dx.x dx.y + XStep div exch XStep div exch % tx ty cmtx a b + 0 YStep dtransform + round exch round exch % tx ty cmtx a b dy.x dy.y + YStep div exch YStep div exch % tx ty cmtx a b c d + 7 -3 roll astore % { a b c d tx ty } + } if + grestore +} bind def +/PATusp { + false PATredef + PATDict begin + CColor PATsc + end +} bind def + +% right45 +11 dict begin +/PaintType 1 def +/PatternType 1 def +/TilingType 1 def +/BBox [0 0 1 1] def +/XStep 1 def +/YStep 1 def +/PatWidth 1 def +/PatHeight 1 def +/Multi 2 def +/PaintData [ + { clippath } bind + { 32 32 true [ 32 0 0 -32 0 32 ] + {<010101010202020204040404080808081010101020202020 + 404040408080808001010101020202020404040408080808 + 101010102020202040404040808080800101010102020202 + 040404040808080810101010202020204040404080808080 + 010101010202020204040404080808081010101020202020 + 4040404080808080>} + imagemask } bind +] def +/PaintProc { + pop + exec fill +} def +currentdict +end +/P5 exch def +1.1111 1.1111 scale %restore scale + +/cp {closepath} bind def +/ef {eofill} bind def +/gr {grestore} bind def +/gs {gsave} bind def +/sa {save} bind def +/rs {restore} bind def +/l {lineto} bind def +/m {moveto} bind def +/rm {rmoveto} bind def +/n {newpath} bind def +/s {stroke} bind def +/sh {show} bind def +/slc {setlinecap} bind def +/slj {setlinejoin} bind def +/slw {setlinewidth} bind def +/srgb {setrgbcolor} bind def +/rot {rotate} bind def +/sc {scale} bind def +/sd {setdash} bind def +/ff {findfont} bind def +/sf {setfont} bind def +/scf {scalefont} bind def +/sw {stringwidth} bind def +/tr {translate} bind def +/tnt {dup dup currentrgbcolor + 4 -2 roll dup 1 exch sub 3 -1 roll mul add + 4 -2 roll dup 1 exch sub 3 -1 roll mul add + 4 -2 roll dup 1 exch sub 3 -1 roll mul add srgb} + bind def +/shd {dup dup currentrgbcolor 4 -2 roll mul 4 -2 roll mul + 4 -2 roll mul srgb} bind def + /DrawEllipse { + /endangle exch def + /startangle exch def + /yrad exch def + /xrad exch def + /y exch def + /x exch def + /savematrix mtrx currentmatrix def + x y tr xrad yrad sc 0 0 1 startangle endangle arc + closepath + savematrix setmatrix + } def + +/$F2psBegin {$F2psDict begin /$F2psEnteredState save def} def +/$F2psEnd {$F2psEnteredState restore end} def +%%EndProlog + +$F2psBegin +10 setmiterlimit +n -1000 6429 m -1000 -1000 l 8005 -1000 l 8005 6429 l cp clip n + 0.06299 0.06299 sc +% Polyline +7.500 slw +n 3060 2070 m 6975 2070 l 6975 5400 l 3060 5400 l cp gs /PC [[0.00 0.82 0.00] [0.00 0.00 0.00]] def 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00000000000..98d503f3de1 --- /dev/null +++ b/Master/texmf-dist/source/latex/hyperref/test/phys2.jpg diff --git a/Master/texmf-dist/source/latex/hyperref/test/picture.eps b/Master/texmf-dist/source/latex/hyperref/test/picture.eps new file mode 100644 index 00000000000..0be39ee9b1d --- /dev/null +++ b/Master/texmf-dist/source/latex/hyperref/test/picture.eps @@ -0,0 +1,311 @@ +%!PS-Adobe-2.0 EPSF-2.0 +%%PDFready: TeXUtil 6.5 - ConTeXt / PRAGMA 1992-1998 +%%BoundingBox: 0 0 36 34 +<< /PageSize [36 34] >> setpagedevice +gsave -44 -525 translate +%%Creator: COREL DRAW +%%Title: CAT.TMP +%%CreationDate: Sat Jan 18 17:29:05 1992 + +%%DocumentFonts: +%%EndComments +%%BeginProlog +% -------------- POSTSCRIPT PROLOG FOR CORELDRAW 2.X ------ +% Copyright Corel Systems Corporation 1990 +/AutoFlatness 0 def/wCorelDict 300 dict def +wCorelDict begin/bd{bind def}bind def/ld{load def}bd +/xd{exch def}bd/_ null def/$c 0 def/$m 0 def +/$y 0 def/$k 0 def/$t 1 def/$n _ def/$o 0 def +/$fil 0 def/$C 0 def/$M 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+\hypersetup{pdfauthor=?`\c C\"asar M\"uller n\~ao!`} +\setcounter{tocdepth}{4} +\setcounter{secnumdepth}{4} +\makeindex +\hypersetup{pdftitle=Welcome to the Monkey House} +\newcommand{\ANS}{\textsf{ANSYS}\xspace} +\begin{document} +\tableofcontents +\section*{Abstract} +\addtocontents{toc}{\protect\addvspace{10pt}} +\addcontentsline{toc}{section}{\protect\numberline{}{ABSTRACT}} +\section{A first, simple, section heading} +And some text +\section{A funny \ANS-section with a \texorpdfstring{$\log$}{log}} +Page 1; See \textcolor{red}{page} --\pageref{page2}-- +\newpage +Page 2; this is page 2\label{page2} +\newpage +\index{an item on page 3} + +\htmladdnormallink{A dummy URL}{http://www.tug.org/A-Fake_URL.html} + +\Acrobatmenu{Quit}{End Acrobat Reader} + +\Acrobatmenu{FullScreen}{Switch to full screen} + +\Acrobatmenu{ZoomIn}{Zoom in} + +$\int\!dx$ +\section{Yet another ?`\c C\"asar M\"uller n\~ao!`} + +\section{Testing Int\'ernal J\oe mps}\label{ss:intjmps} + +This is some text and this is a \hypertarget{target}{target}. + +\newpage + +Now lets jump to \hyperlink{target}{Target}. + +Let's try going to Section~\ref{ss:intjmps} + +\section{A \ss ection with $\leq$} +xx +xx +\subsubsection{A subsubsection \texorpdfstring{$a+b$}{a+b}} +xx +\paragraph{A paragraph} +xx +\subparagraph{A subparagraph} +xxx +Pictures: + +Normal \includegraphics{hog} + +Scaled 0.75 \includegraphics[scale=0.75]{hog} + +Width 1in height 0.5in + \includegraphics[width=1in,height=0.5in]{hog} + +Rotated 50 \includegraphics[scale=0.5,angle=50]{hog} + +Rotated -50 \includegraphics[scale=0.5,angle=-50]{hog} + + +\section{Testing External Jumps}\label{ss:extjmps} + +\begin{enumerate} + +\item Jump to an external: The jump +\href{file:test7#TestTarget}{target} should open test7.pdf on +page 2, +\item Jump to an external: The jump +\href{file:test7#page.1}{page 1} should open test7.pdf on +page 1. + +%\item Jump to an relative external strange file +%\href{/D/srahtz/skills.doc}{destination} + +\href{run:picture.eps}{a PS file to launch} + +\href{run:fontman.exe}{an application} + +\href{run:e:\string\\mdraw\string\\mdraw.exe#picture.eps}{a PS file to launch (2)} +\end{enumerate} +\printindex +\clearpage +\end{document} + + + diff --git a/Master/texmf-dist/source/latex/hyperref/test/test1.tex b/Master/texmf-dist/source/latex/hyperref/test/test1.tex new file mode 100644 index 00000000000..f1894597fee --- /dev/null +++ b/Master/texmf-dist/source/latex/hyperref/test/test1.tex @@ -0,0 +1,328 @@ +\documentclass[11pt]{book} +\makeatletter +\def\listoffigures{\@restonecolfalse\if@twocolumn\@restonecoltrue\onecolumn\fi +\chapter*{List of Figures} +{\let\\ \ \markboth{Title}{List of Figures}} +\addcontentsline{toc}{chapter}{\protect + \numberline{}LIST OF FIGURES}\@starttoc{lof}\if@restonecol \twocolumn\fi} +\makeatother +\usepackage{epsfig,longtable} +\usepackage{makeidx} +\usepackage{varioref} +\usepackage{xr-hyper} +\usepackage{amsmath} +\usepackage[verbose,hypertexnames=false,bookmarksopenlevel=1,bookmarksopen,bookmarksnumbered,colorlinks,plainpages=false,linktocpage]{hyperref} +\def\boldindex#1{\textbf{\hyperpage{#1}}} +\makeindex +\makeatletter +\externaldocument{test2} +\makeatother +%\setcounter{page}{34} +\title{Testing Hyperref} +\author{Sebastian Rahtz} +\date{May 1999} +\setcounter{secnumdepth}{2} +\setcounter{tocdepth}{1} +\begin{document} +\pagenumbering{roman} +% +\makeatletter +\long\def\hyper@section@backref#1#2#3{% + \typeout{BACK REF #1 / #2 / #3}% +\hyperlink{#3}{#2}} +% +\makeatother +\pdfbookmark{Title}{tit} +\setlongtables +\maketitle\index{title} +\tableofcontents +\listoftables +\listoffigures +\pagenumbering{arabic} +\newcommand{\eqnref}[1]{{\autoref{#1}}} +\newtheorem{Argument}{Here we go}[section] +\def\thesubsection{\Roman{section} -- \arabic{subsection}} +\setcounter{tocdepth}{1} + +\chapter[First part]{First part, leading to \protect\autoref{horrid} + next} +\section[Test section]{Our \protect\LaTeX\ test section (leading to \autoref{One}) + for 100\% of \AE horrid $X[Y]Z$ +things, like $42$\label{horrid}} +and so see \autoref{horrid} on page \pageref{horrid}. + +\section{Section One --- cats}\label{One} +see section \vref{Three} about +cats\index{animals!cats} and cite +\cite{Barcelo:1992:caa} + +\section{one.1 -- can we see} +some text with a footnote\footnote{WISH UPON A STAR} +and another one with an extended +footnote\footnote{\protect\label{foot}This is the way the world ends not with a + bang but a whimper. This is the way the world ends not with a + bang but a whimper. This is the way the world ends not with a + bang but a whimper.} +and a reference to a long table\index{tables!long!longtables}, +\autoref{mylongtab}. + +\subsection{one.2} +dogs + +\href{file:test2#page.2}{See page 2 in file test2}, +on page 3 of this file. + +\href{file:test2.pdf#page.2}{See page 2 in file test2.pdf} +on page 3 of this file. + +And can we see \autoref{ss:first} + +in the file test2.pdf? alternatively, +\href{file:test2.pdf#subsection.1.2}{the link like this} + +All Or this? \url{test2.pdf#section.1} + +\newpage +\section{Section Two --- \TeX\ is a dog} +\subsection{two.1} +\subsection{two.2} +\newpage +cite \cite{Barcelo:1992:caa} again. + +\chapter{Second part} +\section{Section Three --- Camels}\label{Three} +see \autoref{One} +\subsection{three.1} + some text with a footnote\footnote{OVER THE RAINBOW} +\index{rainbows} +\subsection{three.2} + +\newpage +\section[Section Four --- Butterflies]{Section Four --- Butterflies and so on} +\subsection{four.1} +\subsection{four.2} +camels +Refer to \hyperref{}{test}{test1}{with these words} +\newpage +\section{Introduction}\label{sec1} +\subsection{subsec} +\newpage +\subsection{subsec}\label{subsec1.2} +Define a marker \hyperdef{test}{test1}{here} while this one is a +PostScript picture acting as marker: +\index{PS pictures} +\hyperlink{testpiccy}{\epsfig{figure=picture,height=1in}} + +This is a picture: \epsfig{figure=picture,height=1in} +\newpage +\section{two}\label{sec2} +\subsection{Subsection 2} +\subsection{Subsection 3} +\newpage +\section{three} +This is a reference to section 1 (\autoref{sec1}), subsection 1.2 +(\autoref{subsec1.2}) and section 2 (\autoref{sec2}). References to +\cite{Barcelo:1992:caa,Dallas:aia}. + + +\begin{figure} + +xxxx + +\hypertarget{testpiccy}{Test picture} + +xxxxx + +xxxxx +\caption{{A cat}} +\label{fig1} +\end{figure} + +\begin{figure} + +xxxx + +xxxxx +\caption{Another cat with a link inside it, +so see \cite{Dallas:aia} xxxx \label{fig2}} +\end{figure} + +\texttt{<<where is \eqnref{eq1}>>} + +\section{Some URLs} + +\begin{minipage}{1.5in} +\url{http://www.aw.com/cp/tlgc.html#Describe} + +\url{http://nsi.net.kiae.su/latex/latex2e.html} + +\url{http://www.lehigh.edu/~dlj0/LyriX.html} + +\url{http://www.cs.wisc.edu/~ghost/index.html} + +\url{http://www.win.tue.nl/win/math/dw/personalpages/dickie/idvi/} + +\url{http://www.tug.org/interest.html#projects} + +\url{ftp://ftp.cbr.dit.csiro.au/staff/gjw/www/tex.html} + + +This is a URL: \url{http://srahtz/attend.html#sebastian} + +\hyperref{file:test2.pdf}{equation}{1}{hello} +\end{minipage} + +\newpage + +\section{Back to math} +\begin{equation} + zzzz + b + \label{eq1} +\end{equation} +and what next? + +\begin{equation} + d - e + \label{eq2} +\end{equation} + +\begin{eqnarray} + y &=&z\\ + g &=&h\\ + \label{eq3} +\end{eqnarray} +We need some lists: +\begin{enumerate} +\item oranges\index{oranges|boldindex} +\item lemons\index{lemons|boldindex} +\item beer\index{beer|boldindex} + \begin{enumerate} + \item Samuel Smiths + \item Labatts + \end{enumerate} +\end{enumerate} + +Lets look at labels in lists: +\begin{enumerate} +\item oranges\label{oranges} +\item lemons\label{lemons} +\item beer\label{beer} + \begin{enumerate} + \item Samuel Smiths\label{smiths} + \item Labatts\label{labatts} + \end{enumerate} +\end{enumerate} +\clearpage + +from which see \autoref{oranges}, \ref{lemons}, \ref{smiths} and +\autoref{labatts} + + +see +sec1: \autoref{sec1} +sec2: \autoref{sec2} +eq1: \autoref{eq1} +fig1: \autoref{fig1} +and cite \cite{Barcelo:1992:caa} again. +\onecolumn +\begin{longtable}{lll} +\caption{A test long table (see \protect\cite{Dallas:aia} +and section \protect\ref{sec1}}\label{mylongtab}\\ +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +a & b & c \\a +\end{longtable} + +% !!! Does not work with hypertexnames=false !!! +Does \hyperref{}{equation}{2.2}{this} point to the second equation? + +Does anything point to the eqnarray (\autoref{eq3})? +\index{cats} + +\begin{thebibliography}{99} +\addcontentsline{toc}{chapter}{Bibliography} +\bibitem{Barcelo:1992:caa} +{Barcel\'o, J.} 1992. +\newblock Programming an intelligent database in archaeology. In \emph{Computer + Applications and Quantitative Methods in Archaeology 1991}, {Lock, G. \& + J.~Moffett} (eds), 21--28, Oxford: British Archaeological Reports. + +\bibitem[Dallas 1992]{Dallas:aia} +{Dallas, C.~J.} 1992. +\newblock Syntax and semantics of figurative art: a formal approach. In + \emph{Archaeology and the Information Age}, {Reilly, P. \& S.~Rahtz} (eds), + chapter~16, London: Routledge. + +\bibitem[Stankovic 1988]{stankovic:88} +J.~Stankovic, ``Misconceptions about real-time computing: a serious problem for + next-generation systems,'' {\em Computer}, vol.~21, no.~10, pp.~10--19, Oct. + 1988. + +\end{thebibliography} + +\clearpage +An index entry for gnus\index{gnus} +\clearpage +An index entry for gnus\index{gnus} +\clearpage +An index entry for gnus\index{gnus} +\clearpage +An index entry for gnus\index{gnus} +\clearpage +An index entry for gnus\index{gnus} +\clearpage +An index entry for gnus\index{gnus} +\chapter*{An appendix --- the Index} +\printindex +\end{document} diff --git a/Master/texmf-dist/source/latex/hyperref/test/test2.tex b/Master/texmf-dist/source/latex/hyperref/test/test2.tex new file mode 100644 index 00000000000..ec8639a9c17 --- /dev/null +++ b/Master/texmf-dist/source/latex/hyperref/test/test2.tex @@ -0,0 +1,63 @@ +\documentclass[reqno]{amsart} +\usepackage{amsfonts} +\usepackage{amssymb} +\usepackage[T1]{fontenc} +\usepackage{ae} +\usepackage{hyperref} + + +\numberwithin{equation}{subsection} + +\begin{document} + +\section{My section title} + +Some text. + +\subsection{My first subsection} +\label{ss:first} + +\begin{equation} +\label{eq:A} +p^{\prime\prime} + \dfrac{S^\prime}{S}p^\prime +k^2p = 0 +\end{equation} + +Let's refer to equations~\ref{eqs:C} in +subsection\ref{ss:second}. + +\begin{equation} +\label{eq:B} +g(x)=const \times f(x) \int^{x} \dfrac{d\xi}{S(\xi)f^{2}(\xi)} . +\end{equation} + +Now I'll force a new page so the hyper-references will bridge a page +boundary. +\newpage + +\subsection{My second subsection} +\label{ss:second} +Now some subequations. + +\begin{subequations} +\label{eqs:C} +\begin{align} +p^\prime& = -Z(x)U \label{eq:pC} \\ +U^\prime & = -Y(x)p \label{eq:UC} +\end{align} +\end{subequations} + +These are related to equation~\ref{eq:A} in subsection~\ref{ss:first}. + +{% +\begin{subequations} +\label{eqs:D} +\begin{align} +p^\prime& = -j \omega {\dfrac{\rho}{S(x)}}U + = -jk {\dfrac{\rho c}{S(x)}}U \label{eq:pD} \\ +U^\prime & = -j \omega {\dfrac{S(x)}{\rho c^{2}}}p + = -jk {\dfrac{S(x)}{\rho c}}p \label{eq:UD} +\end{align} +\end{subequations} +} + +\end{document} diff --git a/Master/texmf-dist/source/latex/hyperref/test/test3.tex b/Master/texmf-dist/source/latex/hyperref/test/test3.tex new file mode 100644 index 00000000000..cbfe6d3a3c7 --- /dev/null +++ b/Master/texmf-dist/source/latex/hyperref/test/test3.tex @@ -0,0 +1,556 @@ +\documentclass{article} +\usepackage{graphicx,ae} +\usepackage[T1]{fontenc} +\usepackage[latin1]{inputenc} +%\def\rmdefault{mbv} +\usepackage{url} +%\textwidth3in +\let\SetRowColor\relax +%\usepackage[times,symbolmenu,spaced=false,zebra,paperwidth=6in,paperheight=4in]{screenpdf} +\usepackage[]{hyperref} +\title{Simulation of Energy Loss Straggling} +\author{Maria Physicist} +\newcommand{\Emax}{\ensuremath{E_{\mathrm{max}}}} +\newcommand{\GEANT}{\texttt{GEANT}} +\begin{document} +\maketitle + +\section{Introduction} + +Due to the statistical nature of ionisation energy loss, large +fluctuations can occur in the amount of energy deposited by a particle +traversing an absorber element. Continuous processes such as multiple +scattering and energy loss play a relevant role in the longitudinal +and lateral development of electromagnetic and hadronic +showers, and in the case of sampling calorimeters the +measured resolution can be significantly affected by such fluctuations +in their active layers. The description of ionisation fluctuations is +characterised by the significance parameter $\kappa$, which is +proportional to the ratio of mean energy loss to the maximum allowed +energy transfer in a single collision with an atomic electron +\[ +\kappa =\frac{\xi}{\Emax} +\] +\Emax{} +is the maximum transferable energy in a single collision with +an atomic electron. +\[ +\Emax =\frac{2 m_e \beta^2\gamma^2 } +{1 + 2\gamma m_e/m_x + \left ( m_e/m_x\right)^2}, +\] +where $\gamma = E/m_x$, $E$ is energy and +$m_x$ the mass of the incident particle, +$\beta^2 = 1 - 1/\gamma^2$ and $m_e$ is the electron mass. +$\xi$ comes from the Rutherford scattering cross section +and is defined as: +\begin{eqnarray*} \xi = \frac{2\pi z^2 e^4 N_{Av} Z \rho \delta x} + {m_e \beta^2 c^2 A} = 153.4 \frac{z^2} {\beta^2} \frac{Z}{A} + \rho \delta x \quad\mathrm{keV}, +\end{eqnarray*} +where + +\begin{tabular}{ll} +\SetRowColor $z$ & charge of the incident particle \\ +\SetRowColor $N_{Av}$ & Avogadro's number \\ +\SetRowColor $Z$ & atomic number of the material \\ +\SetRowColor $A$ & atomic weight of the material \\ +\SetRowColor $\rho$ & density \\ +\SetRowColor $ \delta x$ & thickness of the material \\ +\end{tabular} + +$\kappa$ measures the contribution of the collisions with energy +transfer close to \Emax. For a given absorber, $\kappa$ tends +towards large values if $\delta x$ is large and/or if $\beta$ is +small. Likewise, $\kappa$ tends towards zero if $\delta x $ is small +and/or if $\beta$ approaches 1. + +The value of $\kappa$ distinguishes two regimes which occur in the +description of ionisation fluctuations : + +\begin{enumerate} +\item A large number of collisions involving the loss of all or most + of the incident particle energy during the traversal of an absorber. + + As the total energy transfer is composed of a multitude of small + energy losses, we can apply the central limit theorem and describe + the fluctuations by a Gaussian distribution. This case is + applicable to non-relativistic particles and is described by the + inequality $\kappa > 10 $ (i.e. when the mean energy loss in the + absorber is greater than the maximum energy transfer in a single + collision). + +\item Particles traversing thin counters and incident electrons under + any conditions. + + The relevant inequalities and distributions are $ 0.01 < \kappa < 10 + $, Vavilov distribution, and $\kappa < 0.01 $, Landau distribution. +\end{enumerate} + +An additional regime is defined by the contribution of the collisions +with low energy transfer which can be estimated with the relation +$\xi/I_0$, where $I_0$ is the mean ionisation potential of the atom. +Landau theory assumes that the number of these collisions is high, and +consequently, it has a restriction $\xi/I_0 \gg 1$. In \GEANT{} +(see URL \url{http://wwwinfo.cern.ch/asdoc/geant/geantall.html}), the +limit of Landau theory has been set at $\xi/I_0 = 50$. Below this +limit special models taking into account the atomic structure of the +material are used. This is important in thin layers and gaseous +materials. \autoref{fg:phys332-1} shows the behaviour of $\xi/I_0$ +as a function of the layer thickness for an electron of 100 keV and 1 +GeV of kinetic energy in Argon, Silicon and Uranium. + +\begin{figure} + \centering + \includegraphics[width=.6\linewidth]{phys1} + \caption{The variable $\xi/I_0$ can be used to measure the + validity range of the Landau theory. It depends + on the type and energy of the particle, $Z$, $A$ + and the ionisation potential of the material and + the layer thickness. + } + \label{fg:phys332-1} +\end{figure} + +In the following sections, the different theories and models for the +energy loss fluctuation are described. First, the Landau theory and +its limitations are discussed, and then, the Vavilov and Gaussian +straggling functions and the methods in the thin layers and gaseous +materials are presented. + +\section{Landau theory} +\label{sec:phys332-1} + +For a particle of mass $m_x$ traversing a thickness of material +$\delta x $, the Landau probability distribution may be written in +terms of the universal Landau function $\phi(\lambda)$ +as\cite{bib-LAND}: +\begin{eqnarray*} +f( \epsilon , \delta x ) & = &\frac{1}{\xi} \phi ( \lambda ) +\end{eqnarray*} +where +\begin{eqnarray*} +\phi(\lambda )& = & \frac{1} {2 \pi i}\int^{c+i\infty}_{c-i\infty} +\exp \left ( u \ln u + \lambda u \right ) du \hspace{2cm} c \geq 0 \\ +\lambda & = & \frac{\epsilon -\bar{\epsilon} }{\xi} + - \gamma' - \beta^2 - \ln \frac{\xi}{\Emax} \\ +\gamma' & = & 0.422784\dots = 1 - \gamma \\ +\gamma & = & 0.577215\dots \mbox{(Euler's constant)} \\ +\bar{\epsilon} & = & \mbox{average energy loss} \\ +\epsilon & = & \mbox{actual energy loss} +\end{eqnarray*} + +\subsection{Restrictions} + +The Landau formalism makes two restrictive assumptions : +\begin{enumerate} +\item The typical energy loss is small compared to the maximum energy + loss in a single collision. This restriction is removed in the + Vavilov theory (see \autoref{vavref}). +\item The typical energy loss in the absorber should be large compared + to the binding energy of the most tightly bound electron. For + gaseous detectors, typical energy losses are a few keV which is + comparable to the binding energies of the inner electrons. In such + cases a more sophisticated approach which accounts for atomic energy + levels\cite{bib-TALM} is necessary to accurately simulate data + distributions. In \GEANT, a parameterised model by L. Urb\'{a}n is + used (see section \ref{urban}). +\end{enumerate} + +In addition, the average value of the Landau distribution is infinite. +Summing the Landau fluctuation obtained to the average energy from the +$dE/dx$ tables, we obtain a value which is larger than the one coming +from the table. The probability to sample a large value is small, so +it takes a large number of steps (extractions) for the average +fluctuation to be significantly larger than zero. This introduces a +dependence of the energy loss on the step size which can affect +calculations. + +A solution to this has been to introduce a limit on the value of the +variable sampled by the Landau distribution in order to keep the +average fluctuation to 0. The value obtained from the \texttt{GLANDO} +routine is: +\[ +\delta dE/dx = \epsilon - \bar{\epsilon} = \xi ( \lambda - \gamma' ++\beta^2 +\ln \frac{\xi}{\Emax}) +\] +In order for this to have average 0, we must impose that: +\[ +\bar{\lambda} = -\gamma' - \beta^2 -\ln \frac{\xi}{\Emax} +\] + +This is realised introducing a $\lambda_{\mathrm{max}}(\bar{\lambda})$ +such that if only values of $\lambda \leq \lambda_{\mathrm{max}}$ are +accepted, the average value of the distribution is $\bar{\lambda}$. + +A parametric fit to the universal Landau distribution has been +performed, with following result: +\[ +\lambda_{\mathrm{max}} = 0.60715 + + 1.1934\bar{\lambda}+(0.67794+0.052382\bar{\lambda}) + \exp(0.94753+0.74442\bar{\lambda}) +\] +only values smaller than $\lambda_{\mathrm{max}}$ are accepted, otherwise the +distribution is resampled. + + + +\section{Vavilov theory} +\label{vavref} + +Vavilov\cite{bib-VAVI} derived a more accurate straggling distribution +by introducing the kinematic limit on the maximum transferable energy +in a single collision, rather than using $ \Emax = \infty $. +Now we can write\cite{bib-SCH1}: +\begin{eqnarray*} +f \left ( \epsilon, \delta s \right ) & = & \frac{1}{\xi} \phi_{v} +\left ( \lambda_{v}, \kappa, \beta^{2} \right ) +\end{eqnarray*} +where +\begin{eqnarray*} +\phi_{v} \left ( \lambda_{v}, \kappa, \beta^{2} \right ) & = & +\frac{1}{2 \pi i} \int^{c+i\infty}_{c-i\infty}\phi \left( s \right ) +e^{\lambda s} ds \hspace{2cm} c \geq 0 \\ +\phi \left ( s \right ) & = & +\exp \left [ \kappa ( 1 + \beta^{2}\gamma ) \right ] +~ \exp \left [ \psi \left ( s \right ) \right ], \\ +\psi \left ( s \right ) & = & s \ln \kappa + ( s + \beta^{2} \kappa ) +\left [ \ln (s/\kappa) + E_{1} (s/\kappa) \right ] - \kappa e^{-s/\kappa}, +\end{eqnarray*} +and +\begin{eqnarray*} +E_{1}(z) & = & \int^{\infty}_{z} t^{-1} e^{-t} dt +\mbox{\hspace{1cm} (the exponential integral)} \\ +\lambda_v & = & \kappa \left [ \frac{\epsilon - \bar{\epsilon}}{\xi} +- \gamma' - \beta^2 \right] +\end{eqnarray*} + +The Vavilov parameters are simply related to the Landau parameter by +$\lambda_L = \lambda_v/\kappa - \ln\kappa $. It can be shown that as +$\kappa \rightarrow 0$, the distribution of the variable $\lambda_L$ +approaches that of Landau. For $\kappa \leq 0.01$ the two +distributions are already practically identical. Contrary to what many +textbooks report, the Vavilov distribution \emph{does not} approximate +the Landau distribution for small $\kappa$, but rather the +distribution of $\lambda_L$ defined above tends to the distribution of +the true $\lambda$ from the Landau density function. Thus the routine +\texttt{GVAVIV} samples the variable $\lambda_L$ rather than +$\lambda_v$. For $\kappa \geq 10$ the Vavilov distribution tends to a +Gaussian distribution (see next section). + +\section{Gaussian Theory} + +Various conflicting forms have been proposed for Gaussian straggling +functions, but most of these appear to have little theoretical or +experimental basis. However, it has been shown\cite{bib-SELT} that +for $\kappa \geq 10 $ the Vavilov distribution can be replaced by a +Gaussian of the form : +\begin{eqnarray*} +f( \epsilon , \delta s) \approx \frac{1} +{\xi \sqrt{\frac{2 \pi}{\kappa} \left( 1 - \beta^2/2 \right)}} + \exp \left [ \frac{( \epsilon - \bar{\epsilon} )^2}{2} \frac{\kappa} + {\xi^2 (1- \beta^2/2)}\right ] +\end{eqnarray*} +thus implying +\begin{eqnarray*} +\mathrm{mean} & = & \bar{\epsilon} \\ +\sigma^2 & = & \frac{\xi^2}{\kappa} (1-\beta^2/2) = \xi + \Emax (1-\beta^2/2) +\end{eqnarray*} + +\section{Urb\'an model} +\label{urban} + +The method for computing restricted energy losses with $\delta$-ray +production above given threshold energy in \GEANT{} is a Monte +Carlo method that can be used for thin layers. It is fast and it can +be used for any thickness of a medium. Approaching the limit of the +validity of Landau's theory, the loss distribution approaches smoothly +the Landau form as shown in \autoref{fg:phys332-2}. +\begin{figure} + \centering + \includegraphics[width=.6\linewidth]{phys2} + \caption{Energy loss distribution for a 3 GeV electron in + Argon as given by standard \GEANT. The width of the layers is + given in centimeters.} + \label{fg:phys332-2} +\end{figure} + +It is assumed that the atoms have only two energy levels with binding +energy $E_1$ and $E_2$. The particle--atom interaction will then be +an excitation with energy loss $E_1$ or $E_2$, or an ionisation with +an energy loss distributed according to a function $g(E) \sim 1/E^2$: +\begin{equation} +g(E) = \frac{(\Emax + I)I}{\Emax} \frac{1}{E^2} +\end{equation} + +The macroscopic cross-section for excitations ($i=1,2$) is +\begin{equation} +\label{eq:sigex} +\Sigma_i = C \frac{f_i}{E_i} \frac{\ln (2 m \beta^2 \gamma^2/E_i) - \beta^2} + {\ln (2 m \beta^2 \gamma^2/ I) - \beta^2}(1-r) +\end{equation} +and the macroscopic cross-section for ionisation is +\begin{equation} +\label{eq:sigion} +\Sigma_3 = C \frac{\Emax}{I(\Emax+I) \ln(\frac{\Emax+I}{I})} + ~ r +\end{equation} +\Emax{} is the \GEANT{} cut for $\delta$-production, or the maximum +energy transfer minus mean ionisation energy, if it is smaller than +this cut-off value. The following notation is used: + +\begin{tabular}{ll} +\SetRowColor $r, C$ & parameters of the model \\ +\SetRowColor $E_i$ & atomic energy levels \\ +\SetRowColor $I$ & mean ionisation energy \\ +\SetRowColor ${f_i}$ & oscillator strengths +\end{tabular} + +The model has the parameters $f_i$, $E_i$, $C$ and $r ~(0\leq r\leq +1)$. The oscillator strengths $f_i$ and the atomic level energies +$E_i$ should satisfy the constraints +\begin{eqnarray} +f_1 + f_2 & = & 1 \label{eq:fisum}\\ +f_1 \ln E_1 + f_2 \ln E_2 & = & \ln I \label{eq:flnsum} +\end{eqnarray} +The parameter $C$ can be defined with the help of the mean energy loss +$dE/dx$ in the following way: The numbers of collisions ($n_i$, i = +1,2 for the excitation and 3 for the ionisation) follow the Poisson +distribution with a mean number $ \langle n_i \rangle $. In a step +$\Delta x$ the mean number of collisions is +\begin{equation} +\langle n_i \rangle = \Sigma_i \Delta x +\end{equation} +The mean energy loss $dE/dx$ in a step is the sum of the excitation +and ionisation contributions +\begin{equation} +\frac{dE}{dx} \Delta x = \left[ \Sigma_1 E_1 + \Sigma_2 E_2 + + \Sigma_3 \int_{I}^{\Emax+I} E~g(E)~dE \right] + \Delta x +\end{equation} +From this, using the equations (\ref{eq:sigex}), (\ref{eq:sigion}), +(\ref{eq:fisum}) and (\ref{eq:flnsum}), one can define the parameter +$C$ +\begin{equation} +C = \frac{dE}{dx} +\end{equation} + +The following values have been chosen in \GEANT{} for the other +parameters: +\[ +\begin{array}{lcl} +f_2 = \left\{ \begin{array}{ll} + 0 & \mathrm{if} Z \leq 2 \\ + 2/Z & \mathrm{if} Z > 2 \\ + \end{array} \right. & \Rightarrow & f_1 = 1 - f_2 \\ +E_2 = 10 Z^2 \mathrm{eV} & \Rightarrow & E_1 = \left(\frac{I}{E_{2}^{f_2}} + \right)^{\frac{1}{f_1}} \\ +r = 0.4 & & \\ +\end{array} +\] +With these values the atomic level $E_2$ corresponds approximately +the K-shell energy of the atoms and $Zf_2$ the number of K-shell +electrons. $r$ is the only variable which can be tuned freely. It +determines the relative contribution of ionisation and +excitation to the energy loss. + +The energy loss is computed with the assumption that the step length +(or the relative energy loss) is small, and---in consequence---the +cross-section can be considered constant along the path length. The +energy loss due to the excitation is +\begin{equation} +\Delta E_e = n_1 E_1 + n_2 E_2 +\end{equation} +where $n_1$ and $n_2$ are sampled from Poisson distribution as +discussed above. The loss due to the ionisation can be generated from +the distribution $g(E)$ by the inverse transformation method: +\begin{eqnarray} +u = F(E) & = & \int_{I}^E g(x) dx \nonumber \\ +E = F^{-1}(u) & = & \frac{I}{1 - u \frac {\Emax}{\Emax+I}} \\ +\end{eqnarray} +where $u$ is a uniform random number between $F(I)=0$ and +$F(\Emax+I)=1$. The contribution from the ionisations will be +\begin{equation} +\Delta E_i = \sum_{j=1}^{n_3} \frac{I} + {1 - u_j \frac {\Emax}{\Emax + I}} +\end{equation} +where $n_3$ is the number of ionisation (sampled from Poisson +distribution). The energy loss in a step will then be $\Delta E = +\Delta E_e + \Delta E_i$. + + +\subsection{Fast simulation for $n_3 \geq 16$} + +If the number of ionisation $n_3$ is bigger than 16, a faster sampling +method can be used. The possible energy loss interval is divided in +two parts: one in which the number of collisions is large and the +sampling can be done from a Gaussian distribution and the other in +which the energy loss is sampled for each collision. Let us call the +former interval $[I, \alpha I]$ the interval A, and the latter +$[\alpha I,\Emax]$ the interval B. $\alpha$ lies between 1 and +$\Emax/I$. A collision with a loss in the interval A happens with +the probability +\begin{equation} +\label{eq:phys332-5} +P(\alpha) = \int_I^{\alpha I} g(\!E\!) \, dE = + \frac {( \Emax + I) (\alpha - 1)}{\Emax \alpha} +\end{equation} +The mean energy loss and the standard deviation for this type +of collision are +\begin{equation} +\langle \Delta E(\alpha) \rangle = \frac{1}{P(\alpha)} + \int_I^{\alpha I} E \, g(\!E\!) \, dE = + \frac{I \alpha \ln \alpha}{\alpha - 1} +\end{equation} +and +\begin{equation} +\sigma^2(\alpha) = \frac{1}{P(\alpha)} + \int_I^{\alpha I} E^2 \, g(\!E\!) \, dE = + I^2 \alpha \left( 1 - \frac{\alpha \ln \! ^2 \alpha}{(\alpha - 1)^2} \right) +\end{equation} +If the collision number is high , we assume that the number of the +type A collisions can be calculated from a Gaussian distribution +with the following mean value and standard deviation: +\begin{eqnarray} +\label{eq:phys332-1} +\langle n_A \rangle & = & n_3 P(\alpha) \\ +\label{eq:phys332-2} +\sigma_A^2 & = & n_3 P(\alpha) ( 1 - P(\alpha)) +\end{eqnarray} +It is further assumed that the energy loss in these collisions +has a Gaussian distribution with +\begin{eqnarray} +\label{eq:phys332-3} +\langle \Delta E_A \rangle & = & n_A \langle \Delta E(\alpha) \rangle \\ +\label{eq:phys332-4} +\sigma_{E,A}^2 & = & n_A \sigma^2(\alpha) +\end{eqnarray} +The energy loss of these collision can then be sampled from the +Gaussian distribution. + +The collisions where the energy loss is in the interval B are sampled +directly from +\begin{equation} +\Delta E_B = \sum_{i=1}^{n_3 - n_A} \frac{\alpha I} + {1 - u_i \frac{\Emax + I - \alpha I}{\Emax + I}} +\end{equation} +The total energy loss is the sum of these two types of collisions: +\begin{equation} +\Delta E = \Delta E_A + \Delta E_B +\end{equation} + +The approximation of equations (\ref{eq:phys332-1}), +(\ref{eq:phys332-2}), (\ref{eq:phys332-3}) and (\ref{eq:phys332-4}) +can be used under the following conditions: +\begin{eqnarray} +\label{eq:phys332-6} +\langle n_A \rangle - c \, \sigma_A & \geq & 0 \\ +\label{eq:phys332-7} +\langle n_A \rangle + c \, \sigma_A & \leq & n_3 \\ +\label{eq:phys332-8} +\langle \Delta E_A \rangle - c \, \sigma_{E,A} & \geq & 0 +\end{eqnarray} +where $c \geq 4$. From the equations (\ref{eq:phys332-5}), +(\ref{eq:phys332-1}) and (\ref{eq:phys332-3}) and from the conditions +(\ref{eq:phys332-6}) and (\ref{eq:phys332-7}) the following limits can +be derived: +\begin{equation} +\alpha_{\mathrm{min}} = \frac{(n_3 + c^2)(\Emax+I)} + {n_3 (\Emax + I) + c^2 I} \; \leq \alpha \; \leq +\alpha_{\mathrm{max}} = \frac{(n_3 + c^2)(\Emax+I)} + {c^2 (\Emax + I) + n_3 I} +\end{equation} +This conditions gives a lower limit to number of the ionisations $n_3$ +for which the fast sampling can be done: +\begin{equation} +n_3 \; \geq \; c^2 +\end{equation} +As in the conditions (\ref{eq:phys332-6}), (\ref{eq:phys332-7}) and +(\ref{eq:phys332-8}) the value of $c$ is as minimum 4, one gets $n_3 +\; \geq 16$. In order to speed the simulation, the maximum value is +used for $\alpha$. + +The number of collisions with energy loss in the interval B (the +number of interactions which has to be simulated directly) increases +slowly with the total number of collisions $n_3$. The maximum number +of these collisions can be estimated as +\begin{equation} +n_{B,max} = n_3 - n_{A,min} \approx n_3 (\langle n_A \rangle + - \sigma_A) +\end{equation} +From the previous expressions for $\langle n_A \rangle$ and $\sigma_A$ +one can derive the condition +\begin{equation} +n_B \; \leq \; n_{B,max} = \frac{2 n_3 c^2}{n_3+c^2} +\end{equation} +The following values are obtained with $c=4$: + +\begin{tabular}{llcrr} +$n_3$ & $n_{B,max}$ & & $n_3$ & $n_{B,max}$\\ +\hline +\SetRowColor 16 & 16 & & 200 & 29.63\\ +\SetRowColor 20 & 17.78 & & 500 & 31.01 \\ +\SetRowColor 50 & 24.24 & & 1000 & 31.50 \\ +\SetRowColor 100 & 27.59 & & $\infty$ & 32.00 +\end{tabular} + +\subsection{Special sampling for lower part of the spectrum} + +If the step length is very small ($\leq 5$ mm in gases, $\leq$ 2-3 +$\mu$m in solids) the model gives 0 energy loss for some events. To +avoid this, the probability of 0 energy loss is computed +\begin{equation} +P( \Delta E=0) = e^{-( \langle n_1 \rangle + \langle n_2 \rangle + + \langle n_3 \rangle )} +\end{equation} +If the probability is bigger than 0.01 a special sampling is done, +taking into account the fact that in these cases the projectile +interacts only with the outer electrons of the atom. An energy level +$E_0 = 10$ eV is chosen to correspond to the outer electrons. The mean +number of collisions can be calculated from +\begin{equation} +\langle n \rangle = \frac{1}{E_0} \frac{dE}{dx} \Delta x +\end{equation} +The number of collisions $n$ is sampled from Poisson distribution. +In the case of the thin layers, all the collisions are considered as +ionisations and the energy loss is computed as +\begin{equation} +\Delta E = \sum_{i=1}^n \frac{E_0} + {1 - \frac {\Emax}{\Emax + E_0} u_i} +\end{equation} + + +\begin{thebibliography}{10} +\bibitem{bib-LAND} +L.Landau. +\newblock On the Energy Loss of Fast Particles by Ionisation. +\newblock Originally published in \emph{J. Phys.}, 8:201, 1944. +\newblock Rerpinted in D.ter Haar, Editor, \emph{L.D.Landau, Collected + papers}, page 417. Pergamon Press, Oxford, 1965. + +\bibitem{bib-SCH1} +B.Schorr. +\newblock Programs for the Landau and the Vavilov distributions and the + corresponding random numbers. +\newblock \emph{Comp. Phys. Comm.}, 7:216, 1974. + +\bibitem{bib-SELT} +S.M.Seltzer and M.J.Berger. +\newblock Energy loss straggling of protons and mesons. +\newblock In \emph{Studies in Penetration of Charged Particles in + Matter}, Nuclear Science Series~39, Nat. Academy of Sciences, + Washington DC, 1964. + +\bibitem{bib-TALM} +R.Talman. +\newblock On the statistics of particle identification using ionization. +\newblock \emph{Nucl. Inst. Meth.}, 159:189, 1979. + +\bibitem{bib-VAVI} +P.V.Vavilov. +\newblock Ionisation losses of high energy heavy particles. +\newblock \emph{Soviet Physics JETP}, 5:749, 1957. + +\end{thebibliography} + +\end{document} diff --git a/Master/texmf-dist/source/latex/hyperref/test/test4.tex b/Master/texmf-dist/source/latex/hyperref/test/test4.tex new file mode 100644 index 00000000000..60f6206ee16 --- /dev/null +++ b/Master/texmf-dist/source/latex/hyperref/test/test4.tex @@ -0,0 +1,36 @@ +\documentclass{article} +\usepackage{hyperref} + + +\begin{document} + +\section{My section title} +\include{bit} +\include{bit} +\include{bit} +\include{bit} +\include{bit} +\include{bit} +\include{bit} +\include{bit} +\include{bit} +\include{bit} +\include{bit} +\include{bit} +\include{bit} +\include{bit} +\include{bit} +\include{bit} +\include{bit} +\include{bit} +\include{bit} +\include{bit} +\include{bit} +\include{bit} +\include{bit} +\include{bit} +\include{bit} +\include{bit} +\include{bit} +\include{bit} +\end{document} diff --git a/Master/texmf-dist/source/latex/hyperref/test/test6.tex b/Master/texmf-dist/source/latex/hyperref/test/test6.tex new file mode 100644 index 00000000000..42c80b61de9 --- /dev/null +++ b/Master/texmf-dist/source/latex/hyperref/test/test6.tex @@ -0,0 +1,18 @@ +\documentclass{book} +\usepackage[extension=xxx]{hyperref} +\begin{document} +A\footnote{\texttt{abc}} + +\href{file://localhost/d:/test2.ps}{foo1} + +\href{file://localhost/d:/test2.pdf}{foo2} + +\href{d:/test2.pdf}{foo3} + +\href{d:/test2.ps}{foo4} + +\href{http://www-fourier.ujf-grenoble.fr:80/cgi-bin/zbfr/ZB/math-fr.html?AU=Taylor,+R&format=complete&type=html&maxdocs=10}{weird} + +\href{a%b}{hello} + +\end{document} diff --git a/Master/texmf-dist/source/latex/hyperref/test/test7.tex b/Master/texmf-dist/source/latex/hyperref/test/test7.tex new file mode 100644 index 00000000000..bce6eb5629a --- /dev/null +++ b/Master/texmf-dist/source/latex/hyperref/test/test7.tex @@ -0,0 +1,12 @@ +\documentclass{article} +\usepackage{hyperref} +\usepackage{times} +\begin{document} + +\section{The first section} +hello +\newpage +\section{The second section} +\hypertarget{TestTarget}{goodbye} + +\end{document} diff --git a/Master/texmf-dist/source/latex/hyperref/test/test8.tex b/Master/texmf-dist/source/latex/hyperref/test/test8.tex new file mode 100644 index 00000000000..25a2d3dbfb8 --- /dev/null +++ b/Master/texmf-dist/source/latex/hyperref/test/test8.tex @@ -0,0 +1,41 @@ +% Test file from Stephan Haller <stk@snafu.de> that shows how +% bookmark open levels can vary during the document. + +\documentclass{article} + +\usepackage{times} + +\def\OpMode{1} % fake vtex + +\usepackage{hyperref} + +\begin{document} + +\section{I'm closed (default)} +\subsection{x} + +\hypersetup{bookmarksopen=true} + +\section{I'm open,} +\subsection{and so} +\subsection{are my} +\subsubsection{children} + +\hypersetup{bookmarksopen=false} + +\section{I'm closed,} + +\hypersetup{bookmarksopen=true} + +\subsection{but my} +\subsubsection{children} +\subsection{are} +\subsubsection{open} + +\hypersetup{bookmarksopenlevel=2} + +\section{level is two now} +\subsection{so this is closed} +\subsubsection{y} + +\end{document} diff --git a/Master/texmf-dist/source/latex/hyperref/test/testams.tex b/Master/texmf-dist/source/latex/hyperref/test/testams.tex new file mode 100644 index 00000000000..25e254806b1 --- /dev/null +++ b/Master/texmf-dist/source/latex/hyperref/test/testams.tex @@ -0,0 +1,253 @@ +\documentclass{article} +\usepackage[latin1]{inputenc} +\usepackage{amsmath} +\usepackage{amsfonts} +\usepackage[spanish]{babel} +\usepackage{calc}% or e-TeX, for \hypercalcbp + +\usepackage[% + verbose, + colorlinks=true, + naturalnames=true, + linkcolor=blue, +]{hyperref} + +\addtolength{\topmargin}{-10mm} +\setlength{\oddsidemargin}{-5mm} +\setlength{\evensidemargin}{-5mm} +\setlength{\textwidth}{165mm} +\addtolength{\textheight}{3.5cm} % alargar longitud página + +\hypersetup{% + pdftitle={Notas sobre Control por computador, de Hilario Lopez},% + % Note /XYZ takes three arguments, the X and Y offsets and the + % zoom factor. Omitting these values breaks Distiller. + pdfstartview={% + XYZ \hypercalcbp{1in+\oddsidemargin-2mm} % + \hypercalcbp{\paperheight-1in-\topmargin + -\headheight-\headsep+2mm} % + 1% + }% +} + +% The numbering of the equations is done by the \tag command +% explicitly. Problematic is the equation environment, because +% it generates also an anchor named "equation.1". This would +% produce a lot of warnings. Changing equation to gather +% supresses the warnings. The links should work in both +% cases. +\let\equation\gather +\let\endequation\endgather + +\newcommand{\fdt}{\hbox{f.d.t.\@}} + +\newcommand{\pagina}[1]{\textsl{{\tiny \mbox{[#1]}}}}% << la del fichero grainger-stevenson.tex +\newcommand{\ingles}[1]{\emph{#1}} + + +\newcommand{\ojo}[1]{ } +% +% Crear una caja de texto con borde para destacar ciertos párrafos +% +\newcommand{\destacaP}[1]{ } + + +% +\begin{document} + +\section{Diseño mediante síntesis directa} +Se calculan reguladores por el método de Truxal. +\begin{itemize} + \item Si el proceso tiene un tiempo muerto $d$, el sistema en cadena cerrada no puede + tener un valor menor. +\begin{equation}\label{eq:SintesisDirectaGradosEnBucleCerrado} + gr[L(z)] -gr[N(z)] \ge gr[A(z)]-gr[B(z)] \tag{2.14} +\end{equation} + \item Se obtendrá el mismo tiempo muerto $d$, salvo que en el regulador $G_R$ se + introduzca un nuevo retardo por tener más ceros que polos. + \item Los polos y ceros del proceso externos a la circunferencia unidad no se deben + cancelar con los ceros y polos del regulador, por lo que dichos factores no pueden + aparecer en $G_R(z)$. + \item Asignación de polos (del sistema en cadena cerrada). + Permite especificar (en parte\footnote{Es debido a que los ceros que resulten del regulador + pueden modificar la dinámica que hemos calculado mediante los polos. Habrá que comprobar que + su efecto es despreciable, que implica que los ceros deben ser poco significativos + en comparación con las raíces de $z^2+ \alpha \, z + \beta = 0$} (interesa por tanto que + estén alejados de la circunferencia unidad).) la respuesta transitoria, a + través de un sistema de segundo orden, y poniendo el resto de los polos en $z=0$. + \item Tiempo finito. Todos sus polos están en el origen. Se caracterizan porque alcanzan + el valor final de la respuesta ante una entrada dada en un tiempo finito, + \textsc{sin oscilar la secuencia discreta}. En el caso de control en tiempo real, el + sistema continuo si oscilaría ligeramente. Se refiere a que aunque en los instantes de + muestreo los valores sean los dados por el sistema discreto, el sistema continuo + asociado podría tomar valores distintos entre los instantes de muestreo. + \item Tiempo mínimo. Como los de tiempo finito, pero realizando \textsc{todas} + las cancelaciones \textsc{posibles} (no se consideran posibles las de polos y ceros externos). + \item Respuesta en permanente. Si se desea obtener error de posición nulo y el proceso + no posee un polo en $z=1$, entonces el regulador debe incluir un polo (por lo menos) en + dicho punto. También es necesario esto para eliminar el efecto sobre el permanente de + las perturbaciones deterministas. + \item Simplicidad. Interesa que el número de polos y ceros del regulador sea mínimo. + Esta propiedad es opuesta a la minimización de $m$ (para obtener un sistema de tiempo mínimo). +\end{itemize} +\subsection{Métodos de cálculo} +\subsubsection{Método de asignación de polos} El transitorio puede venir especificado por +$M_p$, $n_p$, y $n_s$. Las fórmulas aplicables son +\begin{align}\label{eq:AsignacionPolosFormulasParametrosTransitorio} + n_p &= \frac{\pi}{\theta} \tag{2.27} \\ + M_p &= |p|^{n_p} \tag{2.28} \\ + n_s &= \frac{\pi}{\sigma} \tag{2.29} \\ + |p| &= e^{-\sigma} \tag{2.30} +\end{align} +La ecuación característica para realimentación unitaria ($H=1$) es +\begin{equation}\label{eq:AsignacionPolosEcuacionCaracteristica} + 1 + G_R(z) \, BG(z) = 0 \tag{2.32} +\end{equation} +o sea +\begin{equation}\label{eq:AsignacionPolosEcuacionCaracteristicaFactorizada} + 1 + \frac{Q(z)}{P(z)} \, \frac{B(z)}{A(z)} = 0 \tag{2.33} +\end{equation} +en la que se observa que puede haber factores que se anulen entre numerador de $G_R$ y +denominador de $G_P$, y viceversa. Operando, resultaría que +\begin{equation}\label{eq:AsignacionPolosEcuacionCaracteristicaNumerador} + A(z) \, P(z) + B(z) \, Q(z) = 0 \tag{2.34} +\end{equation} +% +Debe hacerse notar que si en la ec. +(\ref{eq:AsignacionPolosEcuacionCaracteristicaFactorizada}) se hubiesen anulado factores +entre numerador y denominador, la ecuación +(\ref{eq:AsignacionPolosEcuacionCaracteristicaNumerador}) una vez simplificada sería del +estilo +\begin{equation}\label{eq:AsignacionPolosEcuacionCaracteristicaNumeradorSimplificada} + A'(z) \, P'(z) + B'(z) \, Q'(z) = 0 \tag{2.34-bis} +\end{equation} +en la que $A'(z)$ sería los polos de $A(z)$ que no se cancelan, $B'(z)$ los ceros del +proceso no cancelados (y que por tanto aparecerán en la \fdt de cadena cerrada), y $P'(z)$ +y $Q'(z)$ los polinomios que necesitamos calcular. El factor $Q'(z)$ no se deja como tal, +sino que se pone en función del polinomio $N(z)$, que es el numerador de la \fdt de cadena +cerrada. Para ello se hace uso de la propiedad que dice que los ceros en cadena cerrada +son los del sistema más los del regulador (a menos que se hayan cancelado ceros del +proceso con polos del regulador). +% +La ecuación que debemos plantear para hallar los coeficientes del regulador es +\begin{equation}\label{eq:AsignacionPolosIdentificacionCoeficientes} + z^m (z^2+ \alpha \, z + \beta) = A(z) \, P(z) + B(z) \, Q(z) \tag{2.35} +\end{equation} +% +La solución es única cuando se tengan tantas ecuaciones como incógnitas. Igualando grados, +se tiene que +\begin{equation}\label{eq:AsignacionPolosGradosPolinomios} + m+2 = p+a \tag{2.36} +\end{equation} +y al aplicar la condición (\ref{eq:SintesisDirectaGradosEnBucleCerrado}) a la ecuación +(\ref{eq:AsignacionPolosIdentificacionCoeficientes}) resulta +\begin{equation}\label{AsignacionPolosCondicionGradosBucleCerrado} + (m+2)-n \ge a-b \tag{2.38} +\end{equation} +\subsubsection{Método de tiempo finito} +Todos los polos de cadena cerrada están en el origen ($z=0$). En dichos sistemas, la +respuesta impulsional se puede obtener fácilmente como la secuencia formada por los +coeficientes de $\{b_0, b_1, b_2, \ldots \}$, que es la que resulta de multiplicar la \fdt +por $z^{-m}$, siendo $m$ en número de polos en cadena cerrada (todos en el origen). La +respuesta ante escalón se puede conseguir como suma de la secuencia impulsional: $\{b_0, +b_0+b_1, b_0+b_1+b_2, \ldots \}$. +\ojo{Para los reguladores de tiempo finito, el número de muestras en el origen (valor +cero) coincide con el tiempo muerto, mientras que el número de muestras del transitorio +coincide con el número de ceros. Revisar\pagina{H26} ¿Por que se consideran tres muestras +de transitorio, y no se cuenta la del origen ni la que marca el fin del transitorio, si en +un sistema continuo se contaría todo el tiempo?} +\subsubsection{Método de tiempo mínimo} +Se cancelan todos los polos y ceros de $BG(z)$ interiores a la circunferencia unidad. +\subsection{Mejora del régimen permanente} +Para evitar errores en permanente, puede interesar poner una serie de polos en $z=1$, lo +que se traduce en que en el denominador del regulador habrá un factor $(z-1)^i$, siendo +$G_R$, por tanto, de la forma +\begin{equation}\label{SintesisDirectaPolosEnZIgualAUno} + G_R = \frac{Q(z)}{(z-1)^i \, P(z)} \tag{2.29} +\end{equation} +\subsection{Mejora del régimen transitorio} +Pueden conseguirse respuestas menos bruscas (menor sobreoscilación, etc.) dando más tiempo +para que el sistema se estabilice, lo cual puede conseguirse aumentando $m$ en una unidad, +mientras se mantiene fijo $T_m$, por lo que tendremos un grado de libertad. Otra +posibilidad es poner un filtro entre la señal de consigna y la entrada al bucle de +realimentación, de forma que éste perciba una variación más lenta de la señal de consigna +\pagina{28}. +\subsection{Notas acerca de los problemas propuestos} +\begin{itemize} + \item Son interesantes los ejemplos para ver como se aplican en la práctica las + ecuaciones del estilo a la (\ref{eq:AsignacionPolosIdentificacionCoeficientes}), sobre + todo al cálculo de los valores del grado $n$ y a la aplicación correcta de la + ecuación (\ref{AsignacionPolosCondicionGradosBucleCerrado}). + \item Al incluir integrador en el regulador, la sobreoscilación tiende a aumentar\pagina{40}. + \item Se indica un ejemplo donde se permite incrementar $m$ para obtener el grado de + libertad que nos permita obtener menor sobreoscilación. También se hace uso del + ``truco'' de poner el denominador $z^m$ en la forma $((z-1) + 1)^m$, por lo que haciendo + el desarrollo del binomio de Newton, nos permite poner la \fdt de cadena cerrada como + factores de $(z-1)^k$ en vez de $z^k$, lo que permite simplificar a la hora de igualar + coeficientes, a la vez que garantizamos que no habrá error en permanente, ya que $M(1) = + 1$. + Hay que andarse con ojo si el factor $K$ que multiplica al proceso no es 1 (estando dicho + proceso expresado en la forma de factores $K \cdot \prod (z-c_i)/\prod (z-p_j)$). + En ese caso\pagina{45}, el factor $K$ aparecería multiplicando al cociente de polinomios + que definen $M(z)$ y el coeficiente $n_0$ no sería 1, sino $1/K$. Un ejemplo de este + caso, si se intenta resolver de esta forma, está en el examen del $1^{\textrm{er}}$ parcial + del 25 de Marzo de 1999. +\end{itemize} +\ojo{¿Es cierto que si no se cancelan ceros del proceso, entonces se tiene que la señal de +control $u(k)$ también presenta un comportamiento de tiempo finito? ¿De dónde se deduce +dicha propiedad?} +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\section{Algoritmos de diseño (I)} +\subsection{Algoritmos de tiempo finito (reguladores de Isermann)} +\begin{itemize} + \item La función de transferencia en cadena cerrada no es preespecificada, sino que + viene determinada como resultado del diseño. Todos los polos estarán en el origen. + \item No se cancela ningún cero, pero sí todos los polos. + \item Se incluye integrador, que anula el error en permanente + \item Son muy sencillos de calcular. +\end{itemize} +\subsection{Regulador de tiempo finito de orden normal} +La señal de control $u$ estará estabilizada tras $m$ periodos de muestreo, y la de salida +$y$ tras $m+d$, siendo $d$ el tiempo muerto del proceso. +\subsubsection{Para procesos con tiempo muerto % + \texorpdfstring{$d=0$}{d=0}} +Los coeficientes resultantes para el +regulador son: +\begin{equation}\label{eq:IsermannTiempoFinitoOrdenNormalCoeficientesQCero} + q_0 = \frac{1}{\sum b_i} \tag{3.20a} +\end{equation} +% +\begin{equation}\label{eq:IsermannTiempoFinitoOrdenNormalCoeficientesQi} + q_i = q_0 \, a_i, \quad i=1,\ldots,m + \quad \textrm{(además $\sum q_i = u(m)$, por (3.12, H53))}\tag{3.20b} +\end{equation} +% +\begin{equation}\label{eq:IsermannTiempoFinitoOrdenNormalCoeficientesPi} + p_i = q_0 \, b_i, \quad i=1,\ldots,m + \quad \textrm{(además $\sum p_i = 1$, por (3.11))}\tag{3.20c} +\end{equation} +% +El regulador resultante ($d=0$) es +\begin{equation}\label{eq:IsermannTiempoFinitoOrdenNormalSinTiempoMuerto} + G_R = \frac{Q(z^{-1}))}{1-P(z^{-1}))} = + \frac{q_0 \, A(z^{-1})}{1-q_0 \, B(z^{-1})} \tag{3.21} +\end{equation} +El primer valor de la acción de control es +\begin{equation}\label{eq:IsermannTiempoFinitoOrdenNormalUCero} + u(0) = q_0 = \frac{1}{\sum b_i} \tag{3.22} +\end{equation} + + +\end{document} + +-- ++----------------------------------------------------------------------------+ +| Oscar Fernandez Sierra | +| Escuela Tecnica Superior de Ingenieros Industriales de Gijon | +| Departamento de Construccion e Ingenieria de Fabricacion | +| Campus de Viesques 33204 - Gijon (Spain) | +| | +| E-mail: oscar@charpy.etsiig.uniovi.es Voice: INT +34+ 985.18.22.29/19.30 | +| WWW: http://www1.uniovi.es/ FAX: INT +34+ 985.18.20.55 | ++----------------------------------------------------------------------------+ diff --git a/Master/texmf-dist/source/latex/hyperref/test/testbib.bbl b/Master/texmf-dist/source/latex/hyperref/test/testbib.bbl new file mode 100644 index 00000000000..d1f4e25862c --- /dev/null +++ b/Master/texmf-dist/source/latex/hyperref/test/testbib.bbl @@ -0,0 +1,4 @@ +\begin{thebibliography}{0} +\expandafter\ifx\csname natexlab\endcsname\relax\def\natexlab#1{#1}\fi + +\end{thebibliography} diff --git a/Master/texmf-dist/source/latex/hyperref/test/testbib.bib b/Master/texmf-dist/source/latex/hyperref/test/testbib.bib new file mode 100644 index 00000000000..e2070e7454c --- /dev/null +++ b/Master/texmf-dist/source/latex/hyperref/test/testbib.bib @@ -0,0 +1,27 @@ +@article{Clark:1987, + author = "Adrian Clark", + title = "Halftone output from {\TeX}", + journal = TUB, + volume = "8", + number = "3", + year = "1987", + pages = "270--274" +} + +@unpublished{Clark:1989, + author = "James Clark", + title = "{DVITOPS} User Manual", + year = "1989", + note = "unpublished machine-readable documentation" +} + +@article{Clark:1991, + author = "Adrian Clark", + title = "Practical halftoning with {\TeX}", + journal = TUB, + volume = "12", + number = "1", + year = "1991", + pages = "157--165" +} + diff --git a/Master/texmf-dist/source/latex/hyperref/test/testbib.tex b/Master/texmf-dist/source/latex/hyperref/test/testbib.tex new file mode 100644 index 00000000000..81e8930e567 --- /dev/null +++ b/Master/texmf-dist/source/latex/hyperref/test/testbib.tex @@ -0,0 +1,57 @@ +\errorcontextlines=10 +\documentclass{article} +\usepackage{times} +\usepackage{natbib} +\bibliographystyle{agu} +\usepackage[colorlinks,citecolor=red,pagebackref,hypertexnames=false]{hyperref} +\begin{document} +\title{Another test} +\author{Sergey Lesenko} +\maketitle + +\section{Introduction} +(PDF), described in +\cite{Adobe,Deutsch}, and also available from +\TeX{} $\longrightarrow$ DVIPS\cite{Rokicki} +GhostScript\cite{Deutsch} +TeX2PDF\cite{Sojka} +\cite{Haralambous:TB16-2-162}. We may compare this route with that + +\citeyear{Adobe}, and also available from +\TeX{} $\longrightarrow$ DVIPS\citeyear{Rokicki} +GhostScript\citeyear{Deutsch} +TeX2PDF\citeyear{Sojka} +\citeyear{Haralambous:TB16-2-162}. We may compare this route with that + +\citeauthor{Adobe}, and also available from +\TeX{} $\longrightarrow$ DVIPS\citeauthor{Rokicki} +GhostScript\citeauthor{Deutsch} +TeX2PDF\citeauthor{Sojka} +\citeauthor{Haralambous:TB16-2-162}. We may compare this route with that + +\citefullauthor{Adobe}, and also available from +\TeX{} $\longrightarrow$ DVIPS\citefullauthor{Rokicki} +GhostScript\citefullauthor{Deutsch} +TeX2PDF\citefullauthor{Sojka} +\citefullauthor{Haralambous:TB16-2-162}. We may compare this route with that + +\citet{Adobe}, and also available from +\TeX{} $\longrightarrow$ DVIPS\citet{Rokicki} +GhostScript\citet{Deutsch} +TeX2PDF\citet{Sojka} +\citet{Haralambous:TB16-2-162}. We may compare this route with that + +\citealt{Adobe}, and also available from +\TeX{} $\longrightarrow$ DVIPS\citealt{Rokicki} +GhostScript\citealt{Deutsch} +TeX2PDF\citealt{Sojka} +\citealt{Haralambous:TB16-2-162}. We may compare this route with that + +\cite*{Adobe}, and also available from +\TeX{} $\longrightarrow$ DVIPS\cite*{Rokicki} +GhostScript\cite*{Deutsch} +TeX2PDF\cite*{Sojka} +\cite*{Haralambous:TB16-2-162}. We may compare this route with that + +\bibliography{testbib} +\end{document} diff --git a/Master/texmf-dist/source/latex/hyperref/test/testbmgl.tex b/Master/texmf-dist/source/latex/hyperref/test/testbmgl.tex new file mode 100644 index 00000000000..9fd1684fbf1 --- /dev/null +++ b/Master/texmf-dist/source/latex/hyperref/test/testbmgl.tex @@ -0,0 +1,527 @@ +% testbmgl.tex +% +% Function: +% * How display a pdf reader the bookmarks? +% * Do hyperref.sty and pd1enc.def work properly? +% * Shows the LaTeX code to get the glyphs. +% +% Copyright (c) 1999, 2000, 2008 by Heiko Oberdiek. +% +% This file is part of the `Hyperref Bundle'. +% ------------------------------------------- +% +% 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 later +% version. The latest version of this license is in +% http://www.latex-project.org/lppl.txt +% and version 1.3 or later is part of all distributions of +% LaTeX version 2005/12/01 or later. +% +% This work has the LPPL maintenance status "maintained". +% +% This Current Maintainer of this work is Heiko Oberdiek. +% +% The list of all files belonging to the `Hyperref Bundle' is +% given in the file `manifest.txt'. +% +% Please send error reports and suggestions for improvements to +% Heiko Oberdiek <oberdiek@uni-freiburg.de>. +% +\NeedsTeXFormat{LaTeX2e} +\ProvidesFile{testbmgl.tex}[2008/09/11 v1.3 Test bookmark glyphs (HO)] +\documentclass[12pt,a4paper]{article} +\usepackage[ + bookmarks, + colorlinks, +]{hyperref}[1999/08/31]% v6.65d or later +\pdfstringdefDisableCommands{\let\\\textbackslash} +\IfFileExists{times.sty}{\usepackage{times}}{} +\pagestyle{empty} + +\makeatletter +% from doc.sty: +\def\GetFileInfo#1{% + \def\filename{#1}% + \def\@tempb##1 ##2 ##3\relax##4\relax{% + \def\filedate{##1}% + \def\fileversion{##2}% + \def\fileinfo{##3}% + }% + \edef\@tempa{\csname ver@#1\endcsname}% + \expandafter\@tempb\@tempa\relax? ? \relax\relax +} +\GetFileInfo{testbmgl.tex} +\hypersetup{ + pdftitle={\fileinfo}, + pdfsubject={\filename\space[\filedate\space\fileversion]}, + pdfauthor={Heiko Oberdiek}, + pdfkeywords={bookmarks hyperref PDFDocEncoding glyph slot}, +} + +\edef\BackSlash{\expandafter\@car\string\\\@nil}% +\edef\0{\string\0}% +\edef\1{\string\1}% +\edef\2{\string\2}% +\edef\3{\string\3}% + +\newcommand*\oct[2]{% + \typeout{Processing glyphs #1#20..#1#27}% + \begingroup + \edef\x{\csname#1\endcsname#2}% + \pdfbookmark[1]{#1#20..#1#27: + \_\x0\_\x1\_\x2\_\x3\_\x4\_\x5\_\x6\_\x7\_% + }{#1#2}% + \endgroup +} + +\newcommand*{\@defbookmarkverbcmd}[2]{% + \def#1{#2}% + \edef#1{\expandafter\strip@prefix\meaning#1}% + \edef#1{\expandafter\@removespace#1 \| \|\@nil#1}% + \edef\first{\expandafter\@car#1\@nil}% + \ifx\first\BackSlash + \edef#1{\noexpand\textbackslash\expandafter\@gobble#1}% + \fi +} +\def\@removespace#1 \|#2\@nil#3{\ifx\relax#2\relax#3\else#1\fi} + +\newcounter{alias} +\renewcommand{\thealias}{\alph{alias}} + +% #1#2#3: octal code +% #4: glyph name +% #5: pd1enc-command +\newcommand*\E[6]{% + \setcounter{alias}{0}% + \begingroup + \@defbookmarkverbcmd\x{#5}% + \def\comment{#6}% + \ifx\comment\@empty + \else + \def\comment{ (#6)}% + \fi + \pdfbookmark[2]{% + \textbackslash#1#2#3: + \_\csname#1\endcsname#2#3\_#5\_ + #4 - \x\comment}{#1#2#3}% + \endgroup + \renewcommand*{\alias}[2][]{% + \stepcounter{alias}% + \begingroup + \ifx\relax##1\relax% + \@defbookmarkverbcmd\x{##2}% + \else + \def\x{##1}% + \fi + \pdfbookmark[3]{alias: \_##2\_ \x}{#1#2#3\thealias}% + \endgroup + }% +} +\newcommand*\alias[2][]{} +\newcommand*\e[5]{\E#1#2#3{#4}{#5}{}}% + +\newcommand*\un[3]{% + \pdfbookmark[2]{\textbackslash#1#2#3: unused % + (\_\csname#1\endcsname#2#3\_)}{#1#2#3}% +} + +\newcounter{symlist} +\newcounter{symbol}[symlist] +\newcommand*\symlist[1]{% + \stepcounter{symlist}% + \typeout{Processing symbol list \thesymlist}% + \begingroup + \def\x{\_}% + \@tfor\glyph:=#1\do{% + \expandafter\@addtox\glyph\_\@nil + }% + \pdfbookmark[1]{Symbols: \x}{symbol-\thesymlist}% + \@tfor\glyph:=#1\do{% + \stepcounter{symbol}% + \expandafter\@defbookmarkverbcmd\expandafter\x\expandafter{\glyph}% + \pdfbookmark[2]{\_\glyph\_ \x}{symbol-\thesymlist.\thesymbol}% + }% + \endgroup +} +\def\@addtox#1\@nil{% + \expandafter\def\expandafter\x\expandafter{\x#1}% +} + +\makeatother + +\begin{document} + \oct00 + \un000 + \un001 + \un002 + \un003 + \un004 + \un005 + \un006 + \un007 + \oct01 + \un010 + \e011{horizontal tab}\textHT + \e012{line feed}\textLF + \un013 + \un014 + \e015{carriage return}\textCR + \un016 + \un017 + \oct02 + \un020 + \un021 + \un022 + \un023 + \un024 + \un025 + \un026 + \un027 + \oct03 + \e030{breve}\textasciibreve + \e031{caron}\textasciicaron + \alias{\v{}} + \e032{circumflex}\textcircumflex + \alias{\^{}} + \e033{dotaccent}\textdotaccent + \alias{\.{}} + \e034{hungarumlaut}\texthungarumlaut + \e035{ogonek}\textogonek + \e036{ring}\textring + \alias{\r{}} + \e037{tilde}\texttilde + \alias{\~{}} + \oct04 + \e040{space}\space + \alias[\\\space]\ % + \alias~ + \e041{exclam}! + \e042{quotedbl}\textquotedbl + \e043{numbersign}\textnumbersign + \alias[\textbackslash\#]\# + \e044{dollar}\textdollar + \alias[\textbackslash\$]\$ + \e045{percent}\textpercent + \alias[\textbackslash\%]\% + \e046{ampersand}\textampersand + \alias[\textbackslash\&]\& + \e047{quotesingle}' + \oct05 + \e050{parenleft}\textparenleft + \e051{parenright}\textparenright + \e052{asterisk}* + \e053{plus}+ + \e054{comma}, + \e055{hyphen}- + \e056{period}. + \e057{slash}/ + \oct06 + \e060{zero}0 + \e061{one}1 + \e062{two}2 + \e063{three}3 + \e064{four}4 + \e065{five}5 + \e066{six}6 + \e067{seven}7 + \oct07 + \e070{eight}8 + \e071{nine}9 + \e072{colon}: + \e073{semicolon}; + \e074{less}\textless + \alias< + \e075{equal}= + \e076{greater}\textgreater + \alias> + \e077{question}? + \oct10 + \e100{at}@ + \e101AA + \e102BB + \e103CC + \e104DD + \e105EE + \e106FF + \e107GG + \oct11 + \e110HH + \e111II + \e112JJ + \e113KK + \e114LL + \e115MM + \e116NN + \e117OO + \oct12 + \e120PP + \e121QQ + \e122RR + \e123SS + \e124TT + \e125UU + \e126VV + \e127WW + \oct13 + \e130XX + \e131YY + \e132ZZ + \e133{bracketleft}[ + \e134{backslash}\textbackslash + \alias[\\\\]\\ + \e135{bracketright}] + \e136{asciicircum}\textasciicircum + \e137{underscore}\textunderscore + \alias[\textbackslash\_]\_ + \oct14 + \e140{grave}\textasciigrave + \alias{\`{}} + \e141aa + \e142bb + \e143cc + \e144dd + \e145ee + \e146ff + \e147gg + \oct15 + \e150hh + \e151ii + \e152jj + \e153kk + \e154ll + \e155mm + \e156nn + \e157oo + \oct16 + \e160pp + \e161qq + \e162rr + \e163ss + \e164tt + \e165uu + \e166vv + \e167ww + \oct17 + \e170xx + \e171yy + \e172zz + \e173{braceleft}\textbraceleft + \alias[\textbackslash\{]\{ + \e174{bar}\textbar + \e175{braceright}\textbraceright + \alias[\textbackslash\}]\} + \e176{asciitilde}\textasciitilde + \un177 + \oct20 + \e200{bullet}\textbullet + \e201{dagger}\textdagger + \e202{daggerdbl}\textdaggerdbl + \e203{ellipsis}\textellipsis + \alias\dots + \alias\ldots + \e204{emdash}\textemdash + \e205{endash}\textendash + \e206{florin}\textflorin + \e207{fraction}\textfractionsolidus + \oct21 + \e210{guilsinglleft}\guilsinglleft + \e211{guilsinglright}\guilsinglright + \e212{minus}\textminus + \e213{perthousand}\textperthousand + \e214{quotedblbase}\quotedblbase + \alias\textglqq + \alias\glqq + \e215{quotedblleft}\textquotedblleft + \alias\textgrqq + \alias\grqq + \e216{quotedblright}\textquotedblright + \e217{quoteleft}\textquoteleft + \oct22 + \e220{quoteright}\textquoteright + \e221{quotesinglbase}\quotesinglbase + \e222{trademark}\texttrademark + \e223{fi}\textfi + \e224{fl}\textfl + \e225{Lslash}\L + \e226{OE}\OE + \e227{Scaron}{\v S} + \oct23 + \e230{Ydieresis}{\"Y} + \E231{Zcaron}{\v Z}{PDF 1.3} + \e232{dotlessi}\i + \e233{lslash}\l + \e234{oe}\oe + \e235{scaron}{\v s} + \E236{zcaron}{\v z}{PDF 1.3} + \un237 + \oct24 + \E240{Euro}{\texteuro}{PDF 1.3} + \e241{exclamdown}\textexclamdown + \alias[!{}']{!`} + \e242{cent}\textcent + \e243{sterling}\textsterling + \e244{currency}\textcurrency + \e245{yen}\textyen + \e246{brokenbar}\textbrokenbar + \e247{section}\textsection + \oct25 + \e250{dieresis}\textasciidieresis + \alias{\"{}} + \e251{copyright}\textcopyright + \e252{ordfeminine}\textordfeminine + \e253{guillemotleft}\guillemotleft + \alias\textflqq + \alias\flqq + \e254{logicalnot}\textlogicalnot + \alias\textneg + \un255 + \e256{registered}\textregistered + \e257{macron}\textasciimacron + \oct26 + \e260{degree}\textdegree + \e261{plusminus}\textplusminus + \alias\textpm + \e262{twosuperior}\texttwosuperior + \e263{threesuperior}\textthreesuperior + \e264{acute}\textacute + \alias{\'{}} + \e265{mu}\textmu + \e266{paragraph}\textparagraph + \alias\P + \e267{periodcentered}\textperiodcentered + \alias\textcdot + \oct27 + \e270{cedilla}\textcedilla + \alias{\c{}} + \e271{onesuperior}\textonesuperior + \e272{ordmasculine}\textordmasculine + \e273{guillemotright}\guillemotright + \alias\textfrqq + \alias\frqq + \e274{onequarter}\textonequarter + \e275{onehalf}\textonehalf + \e276{threequarters}\textthreequarters + \e277{questiondown}\textquestiondown + \alias[?{}']{?`} + \oct30 + \e300{Agrave}{\`A} + \e301{Aacute}{\'A} + \e302{Acircumflex}{\^A} + \e303{Atilde}{\~A} + \e304{Adieresis}{\"A} + \e305{Aring}{\r A} + \e306{AE}{\AE} + \e307{Ccedilla}{\c C} + \oct31 + \e310{Egrave}{\`E} + \e311{Eacute}{\'E} + \e312{Ecircumflex}{\^E} + \e313{Edieresis}{\"E} + \e314{Igrave}{\`I} + \e315{Iacute}{\'I} + \e316{Icircumflex}{\^I} + \e317{Idieresis}{\"I} + \oct32 + \e320{Eth}\DH + \alias\DJ + \e321{Ntilde}{\~N} + \e322{Ograve}{\`O} + \e323{Oacute}{\'O} + \e324{Ocircumflex}{\^O} + \e325{Otilde}{\~O} + \e326{Odieresis}{\"O} + \e327{multiply}\textmultiply + \alias\texttimes + \oct33 + \e330{Oslash}\O + \e331{Ugrave}{\`U} + \e332{Uacute}{\'U} + \e333{Ucircumflex}{\^U} + \e334{Udieresis}{\"U} + \e335{Yacute}{\'Y} + \e336{Thorn}\TH + \e337{germandbls}\ss + \alias\textbeta + \oct34 + \e340{agrave}{\`a} + \e341{aacute}{\'a} + \e342{acircumflex}{\^a} + \e343{atilde}{\~a} + \e344{adieresis}{\"a} + \e345{aring}{\r a} + \e346{ae}{\ae} + \e347{ccedilla}{\c c} + \oct35 + \e350{egrave}{\`e} + \e351{eacute}{\'e} + \e352{ecircumflex}{\^e} + \e353{edieresis}{\"e} + \e354{igrave}{\`i} + \alias[\\`\\i]{\`\i} + \e355{iacute}{\'i} + \alias[\\'\\i]{\'\i} + \e356{icircumflex}{\^i} + \alias[\\\textcircumflex\\i]{\^\i} + \e357{idieresis}{\"i} + \alias[\\"\\i]{\"\i} + \oct36 + \e360{eth}\dh + \e361{ntilde}{\~n} + \e362{ograve}{\`o} + \e363{oacute}{\'o} + \e364{ocircumflex}{\^o} + \e365{otilde}{\~o} + \e366{odieresis}{\"o} + \e367{divide}\textdivide + \alias\textdiv + \oct37 + \e370{oslash}\o + \e371{ugrave}{\`u} + \e372{uacute}{\'u} + \e373{ucircumflex}{\^u} + \e374{udieresis}{\"u} + \e375{yacute}{\'y} + \e376{thorn}\th + \e377{ydieresis}{\"y} + \symlist{\SS\textcelsius} + \symlist{\TeX\LaTeX\LaTeXe} + \symlist{\eTeX\MF\MP} + + \section*{\fileinfo} + Document: \textbf{\filename\space[\filedate\space\fileversion]} + \subsection*{Function} + This test file has several tasks: + \begin{itemize} + \item Testing package \emph{hyperref} with encoding file + \emph{pd1enc.def}. + \item Showing glyph commands and aliases that are supported by + package \emph{hyperref}. + \item Test for the pdf reader, especially \emph{AcrobatReader}. + Which glyphs of the \emph{PDFDocEncoding} are + correctly displayed? + \item These glyphs are shown that package \emph{hyperref} + replaces with simpler letters in order to avoid missing glyphs. + \end{itemize} + \subsection*{Short explanation of the bookmarks} + \begin{enumerate} + \item The outline entries of the first level show a summary of their + subentries. Second a screenshot with closed bookmarks + will contain all slots of the \emph{PDFDocEncoding}. + \item The second level of outline entries describes each slot or glyph: + \begin{enumerate} + \item \label{oct}% + Octal code of the slot in the \emph{PDFDocEncoding}. + \item The glyph is shown twice, surrounded by underscores: + The first one is produced by the octal sequence, see \ref{oct}. + The second one is the result of the higher glyph command, + see \ref{high}. + \item The glyph name of \emph{PDFDocEncoding}. + \item \label{high}% + The higher glyph \TeX-command, supported by + package \emph{hyperref}. + \end{enumerate} + \item Aliases of the glyph commands are shown as subentries of the + outline that describes the slot of that glyph command. + \end{enumerate} +\end{document} diff --git a/Master/texmf-dist/source/latex/hyperref/test/testbmu.tex b/Master/texmf-dist/source/latex/hyperref/test/testbmu.tex new file mode 100644 index 00000000000..0de8c2f688a --- /dev/null +++ b/Master/texmf-dist/source/latex/hyperref/test/testbmu.tex @@ -0,0 +1,2017 @@ +% testbmu.tex +% +% Function: +% * How display a pdf reader the bookmarks? +% * Do hyperref.sty and puenc.def work properly? +% * Shows the LaTeX code to get the glyphs. +% +% Copyright (c) 1999, 2000, 2006, 2008 by Heiko Oberdiek. +% +% This file is part of the `Hyperref Bundle'. +% ------------------------------------------- +% +% 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 later +% version. The latest version of this license is in +% http://www.latex-project.org/lppl.txt +% and version 1.3 or later is part of all distributions of +% LaTeX version 2005/12/01 or later. +% +% This work has the LPPL maintenance status "maintained". +% +% This Current Maintainer of this work is Heiko Oberdiek. +% +% The list of all files belonging to the `Hyperref Bundle' is +% given in the file `manifest.txt'. +% +% Please send error reports and suggestions for improvements to +% Heiko Oberdiek <oberdiek@uni-freiburg.de>. +% +\NeedsTeXFormat{LaTeX2e} +\ProvidesFile{testbmu.tex}[2008/09/11 v1.4 Test bookmark glyphs (HO)] +\documentclass[12pt,a4paper]{article} +\usepackage[ + unicode, + bookmarks, + bookmarksopen, + bookmarksopenlevel=0, + colorlinks, +]{hyperref}[1999/08/31]% 6.65d or later +\pdfstringdefDisableCommands{\let\\\textbackslash} +\IfFileExists{times.sty}{\usepackage{times}}{} +\pagestyle{empty} + +\makeatletter +% from doc.sty: +\def\GetFileInfo#1{% + \def\filename{#1}% + \def\@tempb##1 ##2 ##3\relax##4\relax{% + \def\filedate{##1}% + \def\fileversion{##2}% + \def\fileinfo{##3}% + }% + \edef\@tempa{\csname ver@#1\endcsname}% + \expandafter\@tempb\@tempa\relax? ? \relax\relax +} +\GetFileInfo{testbmu.tex} +\hypersetup{ + pdftitle={\fileinfo}, + pdfsubject={\filename\space[\filedate\space\fileversion]}, + pdfauthor={Heiko Oberdiek}, + pdfkeywords={bookmarks hyperref Unicode glyph slot}, +} + +\edef\BackSlash{\expandafter\@car\string\\\@nil}% +\edef\0{\string\0}% +\edef\1{\string\1}% +\edef\2{\string\2}% +\edef\3{\string\3}% +\edef\9{\string\9}% + +\newcommand*\tit[3]{% + \typeout{Unicode high byte #1#2#3}% + \def\highbyte{#1#2#3}% + \def\hb{\9#1#2#3}% + \pdfbookmark[0]{Unicode high byte: #1#2#3}{#1#2#3}% +} + +\newcommand*\oct[2]{% + \typeout{Processing glyphs \highbyte/#1#20..#1#27}% + \begingroup + \edef\x{\hb\csname#1\endcsname#2}% + \pdfbookmark[1]{\highbyte/#1#20..#1#27: + \_\x0\_\x1\_\x2\_\x3\_\x4\_\x5\_\x6\_\x7\_% + }{\highbyte.#1#2}% + \endgroup +} + +\newcommand*{\@defbookmarkverbcmd}[2]{% + \def#1{#2}% + \edef#1{\expandafter\strip@prefix\meaning#1}% + \edef#1{\expandafter\@removespace#1 \| \|\@nil#1}% + \edef\first{\expandafter\@car#1\@nil}% + \ifx\first\BackSlash + \edef#1{\noexpand\textbackslash\expandafter\@gobble#1}% + \fi + \edef#1{\expandafter\@changebackslash\expandafter{#1}}% +} +\def\@removespace#1 \|#2\@nil#3{\ifx\relax#2\relax#3\else#1\fi} +\begingroup + \catcode`\|=0 + \catcode`\\=12 + |gdef|@changebackslash#1{|@@change#1\|END}% + |gdef|@@change#1\#2|END{% + |noexpand#1|@empty + |ifx|\#2|\% + |else + |noexpand|textbackslash + |@removeback#2% + |fi + } + |gdef|@removeback#1\{#1} +|endgroup + +\newcounter{alias} +\renewcommand{\thealias}{\alph{alias}} + +% #1#2#3: octal code +% #4: glyph name +% #5: pd1enc-command +\newcommand*\E[6]{% + \setcounter{alias}{0}% + \begingroup + \@defbookmarkverbcmd\x{#5}% + \def\comment{#6}% + \ifx\comment\@empty + \else + \def\comment{ (#6)}% + \fi + \pdfbookmark[2]{% + \textbackslash#1#2#3: + \_\hb\csname#1\endcsname#2#3\_#5\_ + #4 - \x\comment}{\highbyte.#1#2#3}% + \endgroup + \renewcommand*{\alias}[2][]{% + \stepcounter{alias}% + \begingroup + \ifx\relax##1\relax% + \@defbookmarkverbcmd\x{##2}% + \else + \def\x{##1}% + \fi + \pdfbookmark[3]{alias: \_##2\_ \x}{\highbyte.#1#2#3\thealias}% + \endgroup + }% +} +\newcommand*\alias[2][]{} +\newcommand*\e[5]{\E#1#2#3{#4}{#5}{}}% + +\newcommand*\un[3]{% + \pdfbookmark[2]{\textbackslash#1#2#3: unused % + (\_\hb\csname#1\endcsname#2#3\_)}{\highbyte.#1#2#3}% +} +\newcommand*\na[3]{% + \pdfbookmark[2]{\textbackslash#1#2#3: n. a. % + (\_\hb\csname#1\endcsname#2#3\_)}{\highbyte.#1#2#3}% +} + +\newcounter{symlist} +\newcounter{symbol}[symlist] +\newcommand*\symlist[1]{% + \stepcounter{symlist}% + \typeout{Processing symbol list \thesymlist}% + \begingroup + \def\x{\_}% + \@tfor\glyph:=#1\do{% + \expandafter\@addtox\glyph\_\@nil + }% + \pdfbookmark[1]{Symbols: \x}{symbol-\thesymlist}% + \@tfor\glyph:=#1\do{% + \stepcounter{symbol}% + \expandafter\@defbookmarkverbcmd\expandafter\x\expandafter{\glyph}% + \pdfbookmark[2]{\_\glyph\_ \x}{symbol-\thesymlist.\thesymbol}% + }% + \endgroup +} +\def\@addtox#1\@nil{% + \expandafter\def\expandafter\x\expandafter{\x#1}% +} + +\makeatother + +\begin{document} + \tit000 + \oct00 + \un000 + \un001 + \un002 + \un003 + \un004 + \un005 + \un006 + \un007 + \oct01 + \un010 + \e011{horizontal tab}\textHT + \e012{line feed}\textLF + \un013 + \un014 + \e015{carriage return}\textCR + \un016 + \un017 + \oct02 + \un020 + \un021 + \un022 + \un023 + \un024 + \un025 + \un026 + \un027 + \oct03 + \un030 + \un031 + \un032 + \un033 + \un034 + \un035 + \un036 + \un037 + \oct04 + \e040{space}\space + \alias[\\\space]\ + \alias~ + \e041{exclam}! + \e042{quotedbl}\textquotedbl + \e043{numbersign}\textnumbersign + \alias[\textbackslash\#]\# + \e044{dollar}\textdollar + \alias[\textbackslash\$]\$ + \e045{percent}\textpercent + \alias[\textbackslash\%]\% + \e046{ampersand}\textampersand + \alias[\textbackslash\&]\& + \e047{quotesingle}' + \oct05 + \e050{parenleft}\textparenleft + \e051{parenright}\textparenright + \e052{asterisk}* + \e053{plus}+ + \e054{comma}, + \e055{hyphen}- + \alias\textminus + \e056{period}. + \e057{slash}/ + \oct06 + \e060{zero}0 + \e061{one}1 + \e062{two}2 + \e063{three}3 + \e064{four}4 + \e065{five}5 + \e066{six}6 + \e067{seven}7 + \oct07 + \e070{eight}8 + \e071{nine}9 + \e072{colon}: + \e073{semicolon}; + \e074{less}\textless + \alias< + \e075{equal}= + \e076{greater}\textgreater + \alias> + \e077{question}? + \oct10 + \e100{at}@ + \e101AA + \e102BB + \e103CC + \e104DD + \e105EE + \e106FF + \e107GG + \oct11 + \e110HH + \e111II + \e112JJ + \e113KK + \e114LL + \e115MM + \e116NN + \e117OO + \oct12 + \e120PP + \e121QQ + \e122RR + \e123SS + \e124TT + \e125UU + \e126VV + \e127WW + \oct13 + \e130XX + \e131YY + \e132ZZ + \e133{bracketleft}[ + \e134{backslash}\textbackslash + \alias[\\\\]\\ + \e135{bracketright}] + \e136{asciicircum}\textasciicircum + \e137{underscore}\textunderscore + \alias[\textbackslash\_]\_ + \oct14 + \e140{grave}\textasciigrave + \alias{\`{}} + \e141aa + \e142bb + \e143cc + \e144dd + \e145ee + \e146ff + \e147gg + \oct15 + \e150hh + \e151ii + \alias{\.\i} + \alias{\.i} + \e152jj + \e153kk + \e154ll + \e155mm + \e156nn + \e157oo + \oct16 + \e160pp + \e161qq + \e162rr + \e163ss + \e164tt + \e165uu + \e166vv + \e167ww + \oct17 + \e170xx + \e171yy + \e172zz + \e173{braceleft}\textbraceleft + \alias[\textbackslash\{]\{ + \e174{bar}\textbar + \e175{braceright}\textbraceright + \alias[\textbackslash\}]\} + \e176{asciitilde}\textasciitilde + \na177 + \oct20 + \na200 + \na201 + \na202 + \na203 + \na204 + \na205 + \na206 + \na207 + \oct21 + \na210 + \na211 + \na212 + \na213 + \na214 + \na215 + \na216 + \na217 + \oct22 + \na220 + \na221 + \na222 + \na223 + \na224 + \na225 + \na226 + \na227 + \oct23 + \na230 + \na231 + \na232 + \na233 + \na234 + \na235 + \na236 + \na237 + \oct24 + \na240 + \e241{exclamdown}\textexclamdown + \alias[!{}']{!`} + \e242{cent}\textcent + \e243{sterling}\textsterling + \e244{currency}\textcurrency + \e245{yen}\textyen + \e246{brokenbar}\textbrokenbar + \e247{section}\textsection + \oct25 + \e250{dieresis}\textasciidieresis + \alias{\"{}} + \e251{copyright}\textcopyright + \e252{ordfeminine}\textordfeminine + \e253{guillemotleft}\guillemotleft + \alias\textflqq + \alias\flqq + \e254{logicalnot}\textlogicalnot + \alias\textneg + \un255 + \e256{registered}\textregistered + \e257{macron}\textasciimacron + \oct26 + \e260{degree}\textdegree + \e261{plusminus}\textplusminus + \alias\textpm + \e262{twosuperior}\texttwosuperior + \e263{threesuperior}\textthreesuperior + \e264{acute}\textacute + \alias{\'{}} + \e265{mu}\textmu + \e266{paragraph}\textparagraph + \alias\P + \e267{periodcentered}\textperiodcentered + \alias\textcdot + \oct27 + \e270{cedilla}\textcedilla + \alias{\c{}} + \e271{onesuperior}\textonesuperior + \e272{ordmasculine}\textordmasculine + \e273{guillemotright}\guillemotright + \alias\textfrqq + \alias\frqq + \e274{onequarter}\textonequarter + \e275{onehalf}\textonehalf + \e276{threequarters}\textthreequarters + \e277{questiondown}\textquestiondown + \alias[?{}']{?`} + \oct30 + \e300{Agrave}{\`A} + \e301{Aacute}{\'A} + \e302{Acircumflex}{\^A} + \e303{Atilde}{\~A} + \e304{Adieresis}{\"A} + \e305{Aring}{\r A} + \e306{AE}{\AE} + \e307{Ccedilla}{\c C} + \oct31 + \e310{Egrave}{\`E} + \e311{Eacute}{\'E} + \e312{Ecircumflex}{\^E} + \e313{Edieresis}{\"E} + \e314{Igrave}{\`I} + \e315{Iacute}{\'I} + \e316{Icircumflex}{\^I} + \e317{Idieresis}{\"I} + \oct32 + \e320{Eth}\DH + \alias\DJ + \e321{Ntilde}{\~N} + \e322{Ograve}{\`O} + \e323{Oacute}{\'O} + \e324{Ocircumflex}{\^O} + \e325{Otilde}{\~O} + \e326{Odieresis}{\"O} + \e327{multiply}\textmultiply + \alias\texttimes + \oct33 + \e330{Oslash}\O + \e331{Ugrave}{\`U} + \e332{Uacute}{\'U} + \e333{Ucircumflex}{\^U} + \e334{Udieresis}{\"U} + \e335{Yacute}{\'Y} + \e336{Thorn}\TH + \e337{germandbls}\ss + \alias\textbeta + \oct34 + \e340{agrave}{\`a} + \e341{aacute}{\'a} + \e342{acircumflex}{\^a} + \e343{atilde}{\~a} + \e344{adieresis}{\"a} + \e345{aring}{\r a} + \e346{ae}{\ae} + \e347{ccedilla}{\c c} + \oct35 + \e350{egrave}{\`e} + \e351{eacute}{\'e} + \e352{ecircumflex}{\^e} + \e353{edieresis}{\"e} + \e354{igrave}{\`i} + \alias[\\`\\i]{\`\i} + \e355{iacute}{\'i} + \alias[\\'\\i]{\'\i} + \e356{icircumflex}{\^\i} + \alias[\\^i]{\^i} + \e357{idieresis}{\"i} + \alias[\\"\\i]{\"\i} + \oct36 + \e360{eth}\dh + \e361{ntilde}{\~n} + \e362{ograve}{\`o} + \e363{oacute}{\'o} + \e364{ocircumflex}{\^o} + \e365{otilde}{\~o} + \e366{odieresis}{\"o} + \e367{divide}\textdivide + \alias\textdiv + \oct37 + \e370{oslash}\o + \e371{ugrave}{\`u} + \e372{uacute}{\'u} + \e373{ucircumflex}{\^u} + \e374{udieresis}{\"u} + \e375{yacute}{\'y} + \e376{thorn}\th + \e377{ydieresis}{\"y} + \symlist{\SS} + \symlist{\TeX\LaTeX\LaTeXe} + \symlist{\eTeX\MF\MP} +% + \tit001 + \oct00 + \e000{Amacron}{\=A} + \e001{amacron}{\=a} + \e002{Abreve}{\u A} + \e003{abreve}{\u a} + \e004{Aogonek}{\k A} + \e005{aogonek}{\k a} + \e006{Cacute}{\'C} + \e007{cacute}{\'c} + \oct01 + \e010{Ccircumflex}{\^C} + \e011{ccircumflex}{\^c} + \e012{Cdot}{\.C} + \e013{cdot}{\.c} + \e014{Ccaron}{\v C} + \e015{ccaron}{\v c} + \e016{Dcaron}{\v D} + \e017{dcaron}{\v d} + \oct02 + \e020{Dslash}{\DJ} + \e021{dslash}{\dj} + \e022{Emacron}{\=E} + \e023{emacron}{\=e} + \e024{Ebreve}{\u E} + \e025{ebreve}{\u e} + \e026{Edot}{\.E} + \e027{edot}{\.e} + \oct03 + \e030{Eogonek}{\k E} + \e031{eogonek}{\k e} + \e032{Ecaron}{\v E} + \e033{ecaron}{\v e} + \e034{Gcircumflex}{\^G} + \e035{gcircumflex}{\^g} + \e036{Gbreve}{\u G} + \e037{gbreve}{\u g} + \oct04 + \e040{Gdot}{\.G} + \e041{gdot}{\.g} + \e042{Gcedilla}{\c G} + \e043{gcedilla}{\c g} + \e044{Hcircumflex}{\^H} + \e045{hcircumflex}{\^h} + \e046{Hslash}\textHslash + \e047{hslash}\texthslash + \oct05 + \e050{Itilde}{\~I} + \e051{itilde}{\~i} + \alias[\\~\\i]{\~\i} + \e052{Imacron}{\=I} + \e053{imacron}{\=i} + \alias[\\=\\i]{\=\i} + \e054{Ibreve}{\u I} + \e055{ibreve}{\u i} + \alias[\\u\\i]{\u\i} + \e056{Iogonek}{\k I} + \e057{iogonek}{\k i} + \alias[\\k\\i]{\k\i} + \oct06 + \e060{Idot}{\.I} + \e061{idotless}{\i} + \e062{IJ}{\IJ} + \e063{ij}{\ij} + \e064{Jcircumflex}{\^J} + \e065{jcircumflex}{\^j} + \alias[\\\string^\\j]{\^\j} + \e066{Kcedilla}{\c K} + \e067{kcedilla}{\c k} + \oct07 + \e070{kgreenlandic}\textkra + \e071{Lacute}{\'L} + \e072{lacute}{\'l} + \e073{Lcedilla}{\c L} + \e074{lcedilla}{\c l} + \e075{Lcaron}{\v L} + \e076{lcaron}{\v l} + \na077 + \oct10 + \e100{ldot}{\.l} + \e101{Lslash}{\L} + \e102{lslash}{\l} + \e103{Nacute}{\'N} + \e104{nacute}{\'n} + \e105{Ncedilla}{\c N} + \e106{ncedilla}{\c n} + \e107{Ncaron}{\v N} + \oct11 + \e110{ncaron}{\v n} + \e111{napostrope}\textnapostrophe + \e112{NG}\NG + \e113{ng}\ng + \e114{Omacron}{\=O} + \e115{omacron}{\=o} + \e116{Obreve}{\u O} + \e117{obreve}{\u o} + \oct12 + \e120{Odoubleacute}{\H O} + \e121{odoubleacute}{\H o} + \e122{OE}{\OE} + \e123{oe}{\oe} + \e124{Racute}{\'R} + \e125{racute}{\'r} + \e126{Rcedilla}{\c R} + \e127{rcedilla}{\c r} + \oct13 + \e130{Rcaron}{\v R} + \e131{rcaron}{\v r} + \e132{Sacute}{\'S} + \e133{sacute}{\'s} + \e134{Scircumflex}{\^S} + \e135{scircumflex}{\^s} + \e136{Scedilla}{\c S} + \e137{scedilla}{\c s} + \oct14 + \e140{Scaron}{\v S} + \e141{scaron}{\v s} + \e142{Tcedilla}{\c T} + \e143{tcedilla}{\c t} + \e144{Tcaron}{\v T} + \e145{tcaron}{\v t} + \e146{Tslash}{\textTslash} + \e147{tslash}{\texttslash} + \oct15 + \e150{Utilde}{\~U} + \e151{utilde}{\~u} + \e152{Umacron}{\=U} + \e153{umacron}{\=u} + \e154{Ubreve}{\u U} + \e155{ubreve}{\u u} + \e156{Uring}{\r U} + \e157{uring}{\r u} + \oct16 + \e160{Udoubleacute}{\H U} + \e161{udoubleacute}{\H u} + \e162{Uogonek}{\k U} + \e163{uogonek}{\k u} + \e164{Wcircumflex}{\^W} + \e165{wcircumflex}{\^w} + \e166{Ycircumflex}{\^Y} + \e167{ycircumflex}{\^y} + \oct17 + \e170{Ydieresis}{\"Y} + \e171{Zacute}{\'Z} + \e172{zacute}{\'z} + \e173{Zdot}{\.Z} + \e174{zdot}{\.z} + \e175{Zcaron}{\v Z} + \e176{zcaron}{\v z} + \e177{longs}\textlongs + \oct20 + \na200 + \na201 + \na202 + \na203 + \na204 + \na205 + \na206 + \na207 + \oct21 + \na210 + \na211 + \na212 + \na213 + \na214 + \na215 + \na216 + \na217 + \oct22 + \na220 + \na221 + \e222{florin}\textflorin + \na223 + \na224 + \na225 + \na226 + \na227 + \oct23 + \na230 + \na231 + \na232 + \na233 + \na234 + \na235 + \na236 + \na237 + \oct24 + \na240 + \na241 + \na242 + \na243 + \na244 + \na245 + \na246 + \na247 + \oct25 + \na250 + \na251 + \na252 + \na253 + \na254 + \na255 + \na256 + \na257 + \oct26 + \na260 + \na261 + \na262 + \na263 + \na264 + \na265 + \na266 + \na267 + \oct27 + \na270 + \na271 + \na272 + \na273 + \na274 + \na275 + \na276 + \na277 + \oct30 + \na300 + \na301 + \na302 + \na303 + \na304 + \na305 + \na306 + \na307 + \oct31 + \na310 + \na311 + \na312 + \na313 + \na314 + \e315{Acaron}{\v A} + \e316{acaron}{\v a} + \e317{Icaron}{\v I} + \oct32 + \e320{icaron}{\v i} + \alias[\\v\\i]{\v\i} + \e321{Ocaron}{\v O} + \e322{ocaron}{\v o} + \e323{Ucaron}{\v U} + \e324{ucaron}{\v u} + \na325 + \na326 + \na327 + \oct33 + \na330 + \na331 + \na332 + \na333 + \na334 + \na335 + \na336 + \na337 + \oct34 + \na340 + \na341 + \na342 + \na343 + \e344{Gslash}{\textGslash} + \e345{gslash}{\textgslash} + \e346{Gcaron}{\v G} + \e347{gcaron}{\v g} + \oct35 + \e350{Kcaron}{\v K} + \e351{kcaron}{\v k} + \e352{Oogonek}{\k O} + \e353{oogonek}{\k o} + \na354 + \na355 + \na356 + \na357 + \oct36 + \e360{jcaron}{\v\j} + \alias{\v j} + \na361 + \na362 + \na363 + \e364{Gacute}{\'G} + \e365{gacute}{\'g} + \na366 + \na367 + \oct37 + \e370{N with grave}{\`N} + \e371{n with grave}{\`n} + \na372 + \na373 + \e374{AE with acute}{\'\AE} + \e375{ae with acute}{\'\ae} + \e376{O with stroke and acute}{\'\O} + \e377{o with stroke and acute}{\'\o} +% + \tit002 + \oct00 + \na000 + \na001 + \na002 + \na003 + \na004 + \na005 + \na006 + \na007 + \oct01 + \na010 + \na011 + \na012 + \na013 + \na014 + \na015 + \na016 + \na017 + \oct02 + \na020 + \na021 + \na022 + \na023 + \na024 + \na025 + \na026 + \na027 + \oct03 + \na030 + \na031 + \na032 + \na033 + \na034 + \na035 + \na036 + \na037 + \oct04 + \na040 + \na041 + \na042 + \na043 + \na044 + \na045 + \na046 + \na047 + \oct05 + \na050 + \na051 + \na052 + \na053 + \na054 + \na055 + \na056 + \na057 + \oct06 + \na060 + \na061 + \na062 + \na063 + \na064 + \na065 + \na066 + \na067 + \oct07 + \na070 + \na071 + \na072 + \na073 + \na074 + \na075 + \na076 + \na077 + \oct10 + \na100 + \na101 + \na102 + \na103 + \na104 + \na105 + \na106 + \na107 + \oct11 + \na110 + \na111 + \na112 + \na113 + \na114 + \na115 + \na116 + \na117 + \oct12 + \na120 + \na121 + \na122 + \na123 + \na124 + \na125 + \na126 + \na127 + \oct13 + \na130 + \na131 + \na132 + \na133 + \na134 + \na135 + \na136 + \na137 + \oct14 + \na140 + \na141 + \na142 + \na143 + \na144 + \na145 + \na146 + \na147 + \oct15 + \na150 + \na151 + \na152 + \na153 + \na154 + \na155 + \na156 + \na157 + \oct16 + \na160 + \na161 + \na162 + \na163 + \na164 + \na165 + \na166 + \na167 + \oct17 + \na170 + \na171 + \na172 + \na173 + \na174 + \na175 + \na176 + \na177 + \oct20 + \na200 + \na201 + \na202 + \na203 + \na204 + \na205 + \na206 + \na207 + \oct21 + \na210 + \na211 + \na212 + \na213 + \na214 + \na215 + \na216 + \na217 + \oct22 + \na220 + \na221 + \na222 + \na223 + \na224 + \na225 + \na226 + \na227 + \oct23 + \na230 + \na231 + \na232 + \na233 + \na234 + \na235 + \na236 + \na237 + \oct24 + \na240 + \na241 + \na242 + \na243 + \na244 + \na245 + \na246 + \na247 + \oct25 + \na250 + \na251 + \na252 + \na253 + \na254 + \na255 + \na256 + \na257 + \oct26 + \na260 + \na261 + \na262 + \na263 + \na264 + \na265 + \na266 + \na267 + \oct27 + \na270 + \na271 + \na272 + \na273 + \na274 + \na275 + \na276 + \na277 + \oct30 + \na300 + \na301 + \na302 + \na303 + \na304 + \na305 + \na306 + \na307 + \oct31 + \na310 + \na311 + \na312 + \na313 + \na314 + \na315 + \na316 + \na317 + \oct32 + \na320 + \na321 + \na322 + \na323 + \na324 + \na325 + \na326 + \na327 + \oct33 + \na330 + \na331 + \na332 + \na333 + \na334 + \na335 + \na336 + \na337 + \oct34 + \na340 + \na341 + \na342 + \na343 + \na344 + \na345 + \na346 + \na347 + \oct35 + \na350 + \na351 + \na352 + \na353 + \na354 + \na355 + \na356 + \na357 + \oct36 + \na360 + \na361 + \na362 + \na363 + \na364 + \na365 + \na366 + \na367 + \oct37 + \na370 + \na371 + \na372 + \na373 + \na374 + \na375 + \na376 + \na377 +% + \tit003 + \oct00 + \na000 + \na001 + \na002 + \na003 + \na004 + \na005 + \na006 + \na007 + \oct01 + \na010 + \na011 + \na012 + \na013 + \na014 + \na015 + \na016 + \na017 + \oct02 + \na020 + \na021 + \na022 + \na023 + \na024 + \na025 + \na026 + \na027 + \oct03 + \na030 + \na031 + \na032 + \na033 + \na034 + \na035 + \na036 + \na037 + \oct04 + \na040 + \na041 + \na042 + \na043 + \na044 + \na045 + \na046 + \na047 + \oct05 + \na050 + \na051 + \na052 + \na053 + \na054 + \na055 + \na056 + \na057 + \oct06 + \na060 + \na061 + \na062 + \na063 + \na064 + \na065 + \na066 + \na067 + \oct07 + \na070 + \na071 + \na072 + \na073 + \na074 + \na075 + \na076 + \na077 + \oct10 + \na100 + \na101 + \na102 + \na103 + \na104 + \na105 + \na106 + \na107 + \oct11 + \na110 + \na111 + \na112 + \na113 + \na114 + \na115 + \na116 + \na117 + \oct12 + \na120 + \na121 + \na122 + \na123 + \na124 + \na125 + \na126 + \na127 + \oct13 + \na130 + \na131 + \na132 + \na133 + \na134 + \na135 + \na136 + \na137 + \oct14 + \na140 + \na141 + \na142 + \na143 + \na144 + \na145 + \na146 + \na147 + \oct15 + \na150 + \na151 + \na152 + \na153 + \na154 + \na155 + \na156 + \na157 + \oct16 + \na160 + \na161 + \na162 + \na163 + \na164 + \na165 + \na166 + \na167 + \oct17 + \na170 + \na171 + \na172 + \na173 + \na174 + \na175 + \na176 + \na177 + \oct20 + \na200 + \na201 + \na202 + \na203 + \na204 + \na205 + \e206{Alpha tonos}{\'\textAlpha} + \na207 + \oct21 + \e210{Epsilon tonos}{\'\textEpsilon} + \e211{Eta tonos}{\'\textEta} + \e212{Iota tonos}{\'\textIota} + \na213 + \e214{Omicron tonos}{\'\textOmicron} + \na215 + \e216{Upsilon tonos}{\'\textUpsilon} + \e217{Omega tonos}{\'\textOmega} + \oct22 + \e220{Iota dialytika tonos}{\'\textIotadieresis} + \e221{Alpha}\textAlpha + \e222{Beta}\textBeta + \e223{Gamma}\textGamma + \e224{Delta}\textDelta + \e225{Epsilon}\textEpsilon + \e226{Zeta}\textZeta + \e227{Eta}\textEta + \oct23 + \e230{Theta}\textTheta + \e231{Iota}\textIota + \e232{Kappa}\textKappa + \e233{Lambda}\textLambda + \e234{Mu}\textMu + \e235{Nu}\textNu + \e236{Xi}\textXi + \e237{Omicron}\textOmicron + \oct24 + \e240{Pi}\textPi + \e241{Rho}\textRho + \na242 + \e243{Sigma}\textSigma + \e244{Tau}\textTau + \e245{Upsilon}\textUpsilon + \e246{Phi}\textPhi + \e247{Chi}\textChi + \oct25 + \e250{Psi}\textPsi + \e251{Omega}\textOmega + \e252{Iota dialytika}{\"\textIota} + \e253{Upsilon dialytika}{\"\textUpsilon} + \e254{alpha tonos}{\'\textalpha} + \e255{epsilon tonos}{\'\textepsilon} + \e256{eta tonos}{\'\texteta} + \e257{iota tonos}{\'\textiota} + \oct26 + \e260{upsilon dialytika tonos}{\"\textupsilonacute} + \e261{alpha}\textalpha + \e262{beta}\textbeta + \e263{gamma}\textgamma + \e264{delta}\textdelta + \e265{epsilon}\textepsilon + \e266{zeta}\textzeta + \e267{eta}\texteta + \oct27 + \e270{theta}\texttheta + \e271{iota}\textiota + \e272{kappa}\textkappa + \e273{lambda}\textlambda + \e274{mu}\textmu + \e275{nu}\textnu + \e276{xi}\textxi + \e277{omicron}\textomicron + \oct30 + \e300{pi}\textpi + \e301{rho}\textrho + \e302{varsigma}\textvarsigma + \e303{sigma}\textsigma + \e304{tau}\texttau + \e305{upsilon}\textupsilon + \e306{phi}\textphi + \e307{chi}\textchi + \oct31 + \e310{psi}\textpsi + \e311{omega}\textomega + \e312{iota dialytika}{\"\textiota} + \e313{upsilon dialytika}{\"\textupsilon} + \e314{omicron tonos}{\'\textomicron} + \e315{upsilon tonos}{\'\textupsilon} + \e316{omega tonos}{\'\textomega} + \na317 + \oct32 + \na320 + \na321 + \na322 + \na323 + \na324 + \na325 + \na326 + \na327 + \oct33 + \na330 + \na331 + \na332 + \na333 + \na334 + \na335 + \na336 + \na337 + \oct34 + \na340 + \na341 + \na342 + \na343 + \na344 + \na345 + \na346 + \na347 + \oct35 + \na350 + \na351 + \na352 + \na353 + \na354 + \na355 + \na356 + \na357 + \oct36 + \na360 + \na361 + \na362 + \na363 + \na364 + \na365 + \na366 + \na367 + \oct37 + \na370 + \na371 + \na372 + \na373 + \na374 + \na375 + \na376 + \na377 +% + \tit004 + \oct00 + \na000 + \e001{IO}\CYRYO + \alias[\\"\\CYRE]{\"\CYRE} + \e002{DJE}\CYRDJE + \e003{GJE}{\'\CYRG} + \e004{ukrainian IE}\CYRIE + \e005{DZE}\CYRDZE + \e006{byelorussian-ukrainian I}\CYRII + \e007{YI}\CYRYI + \oct01 + \e010{JE}\CYRJE + \e011{LJE}\CYRLJE + \e012{NJE}\CYRNJE + \e013{TSHE}\CYRTSHE + \e014{KJE}{\'\CYRK} + \na015 + \e016{short U}\CYRUSHRT + \e017{DZHE}\CYRDZHE + \oct02 + \e020{A}\CYRA + \e021{BE}\CYRB + \e022{VE}\CYRV + \e023{GHE}\CYRG + \e024{DE}\CYRD + \e025{IE}\CYRE + \e026{ZHE}\CYRZH + \e027{ZE}\CYRZ + \oct03 + \e030{I}\CYRI + \e031{short I}\CYRISHRT + \alias[\\U\\CYRI]{\U\CYRI} + \e032{KA}\CYRK + \e033{EL}\CYRL + \e034{EM}\CYRM + \e035{EN}\CYRN + \e036{O}\CYRO + \e037{PE}\CYRP + \oct04 + \e040{ER}\CYRR + \e041{ES}\CYRS + \e042{TE}\CYRT + \e043{U}\CYRU + \e044{EF}\CYRF + \e045{HA}\CYRH + \e046{TSE}\CYRC + \e047{CHE}\CYRCH + \oct05 + \e050{SHA}\CYRSH + \e051{SHCHA}\CYRSHCH + \e052{HARD SIGN}\CYRHRDSN + \e053{YERU}\CYRERY + \e054{SOFT SIGN}\CYRSFTSN + \e055{E}\CYREREV + \e056{YU}\CYRYU + \e057{YA}\CYRYA + \oct06 + \e060{a}\cyra + \e061{be}\cyrb + \e062{ve}\cyrv + \e063{ghe}\cyrg + \e064{de}\cyrd + \e065{ie}\cyre + \e066{zhe}\cyrzh + \e067{ze}\cyrz + \oct07 + \e070{i}\cyri + \e071{short i}\cyrishrt + \alias[\\U\\cyri]{\U\cyri} + \e072{ka}\cyrk + \e073{el}\cyrl + \e074{em}\cyrm + \e075{en}\cyrn + \e076{o}\cyro + \e077{pe}\cyrp + \oct10 + \e100{er}\cyrr + \e101{es}\cyrs + \e102{te}\cyrt + \e103{u}\cyru + \e104{ef}\cyrf + \e105{ha}\cyrh + \e106{tse}\cyrc + \e107{che}\cyrch + \oct11 + \e110{sha}\cyrsh + \e111{shcha}\cyrshch + \e112{hard sign}\cyrhrdsn + \e113{yeru}\cyrery + \e114{soft sign}\cyrsftsn + \e115{e}\cyrerev + \e116{yu}\cyryu + \e117{ya}\cyrya + \oct12 + \na120 + \e121{io}\cyryo + \e122{dje}\cyrdje + \e123{gje}{\'\cyrg} + \e124{ukrainian ie}\cyrie + \e125{dze}\cyrdze + \e126{byelorussian-ukrainian i}\cyrii + \e127{yi}\cyryi + \oct13 + \e130{je}\cyrje + \e131{lje}\cyrlje + \e132{nje}\cyrnje + \e133{tshe}\cyrtshe + \e134{kje}{\'\cyrk} + \na135 + \e136{short u}\cyrushrt + \e137{dzhe}\cyrdzhe + \oct14 + \e140{OMEGA}\CYROMEGA + \e141{omega}\cyromega + \e142{YAT}\CYRYAT + \e143{yat}\cyryat + \e144{iotified E}\CYRIOTE + \e145{iotified e}\cyriote + \e146{little YUS}\CYRLYUS + \e147{little yus}\cyrlyus + \oct15 + \e150{iotified little YUS}\CYRIOTLYUS + \e151{iotified little yos}\cyriotlyus + \e152{big YUS}\CYRBYUS + \e153{big yus}\cyrbyus + \e154{iotified big YUS}\CYRIOTBYUS + \e155{iotified big yus}\cyriotbyus + \e156{KSI}\CYRKSI + \e157{ksi}\cyrksi + \oct16 + \e160{PSI}\CYRPSI + \e161{psi}\cyrpsi + \e162{FITA}\CYRFITA + \e163{fita}\cyrfita + \e164{IZHISA}\CYRIZH + \e165{izhisa}\cyrizh + \e166{IZHISA double grave}{\C\CYRIZH} + \e167{izhisa double grave}{\C\cyrizh} + \oct17 + \e170{UK}\CYRUK + \e171{uk}\cyruk + \e172{round OMEGA}\CYROMEGARND + \e173{round omega}\cyromegarnd + \e174{OMEGA titlo}\CYROMEGATITLO + \e175{omega titlo}\cyromegatitlo + \e176{OT}\CYROT + \e177{ot}\cyrot + \oct20 + \e200{KOPPA}\CYRKOPPA + \e201{koppa}\cyrkoppa + \e202{thousands sign}\cyrthousands + \na203 + \na204 + \na205 + \na206 + \na207 + \oct21 + \na210 + \na211 + \na212 + \na213 + \na214 + \na215 + \na216 + \na217 + \oct22 + \e220{GHE upturn}\CYRGUP + \e221{ghe upturn}\cyrgup + \e222{GHE stroke}\CYRGHCRS + \e223{ghe stroke}\cyrghcrs + \e224{GHE middle hook}\CYRGHK + \e225{ghe middle hook}\cyrghk + \e226{ZHE descender}\CYRZHDSC + \e227{zhe descender}\cyrzhdsc + \oct23 + \e230{ZE descender}\CYRZDSC + \e231{ze descender}\cyrzdsc + \e232{KA descender}\CYRKDSC + \e233{ka descender}\cyrkdsc + \e234{KA vertical stroke}\CYRKVCRS + \e235{ka vertical stroke}\cyrkvcrs + \e236{KA stroke}\CYRKHCRS + \e237{ka stroke}\cyrkhcrs + \oct24 + \e240{bashkir KA}\CYRKBEAK + \e241{bashkir ka}\cyrkbeak + \e242{EN descender}\CYRNDSC + \e243{en descender}\cyrndsc + \e244{ligature EN GHE}\CYRNG + \e245{ligature en ghe}\cyrng + \e246{PE middle hook}\CYRPHK + \e247{pe middle hook}\cyrphk + \oct25 + \e250{abkhasian HA}\CYRABHHA + \e251{abkhasian ha}\cyrabhha + \e252{ES descender}\CYRSDSC + \e253{es descender}\cyrsdsc + \e254{TE descender}\CYRTDSC + \e255{te descender}\cyrtdsc + \e256{straight U}\CYRY + \e257{straight u}\cyry + \oct26 + \e260{straight U stroke}\CYRYHCRS + \e261{straight u stroke}\cyryhcrs + \e262{HA descender}\CYRHDSC + \e263{ha descender}\cyrhdsc + \e264{ligature TE TSE}\CYRTETSE + \e265{ligature te tse}\cyrtetse + \e266{CHE right descender}\CYRCHRDSC + \e267{che right descender}\cyrchrdsc + \oct27 + \e270{CHE vertical stroke}\CYRCHVCRS + \e271{che vertical stroke}\cyrchvcrs + \e272{SHHA}\CYRSHHA + \e273{shha}\cyrshha + \e274{abkhasian CHE}\CYRABHCH + \e275{abkhasian che}\cyrabhch + \e276{abkhasian CHE descender}\CYRABHCHDSC + \e277{abkhasian che descender}\cyrabhchdsc + \oct30 + \e300{palochka}\CYRpalochka + \e301{ZHE breve}{\U\CYRZH} + \e302{zhe breve}{\U\cyrzh} + \e303{KA hook}\CYRKHK + \e304{ka hook}\cyrkhk + \na305 + \na306 + \e307{EN hook}\CYRNHK + \oct31 + \e310{en hook}\cyrnhk + \na311 + \na312 + \e313{khakassian CHE}\CYRCHLDSC + \e314{khakassian che}\cyrchldsc + \na315 + \na316 + \na317 + \oct32 + \e320{A breve}{\U\CYRA} + \e321{a breve}{\U\cyra} + \e322{A diaeresis}{\"\CYRA} + \e323{a diaeresis}{\"\cyra} + \e324{ligature A IE}\CYRAE + \e325{ligature a ie}\cyrae + \e326{IE breve}{\U\CYRE} + \e327{ie breve}{\U\cyre} + \oct33 + \e330{SCHWA}\CYRSCHWA + \e331{schwa}\cyrschwa + \e332{SCHWA diaeresis}{\"\CYRSCHWA} + \e333{schwa diaeresis}{\"\cyrschwa} + \e334{ZHE diaeresis}{\"\CYRZH} + \e335{zhe diaeresis}{\"\cyrzh} + \e336{ZE diaeresis}{\"\CYRZ} + \e337{ze diaeresis}{\"\cyrz} + \oct34 + \e340{abkhasian DZE}\CYRABHDZE + \e341{abkhasian dze}\cyrabhdze + \e342{I macron}{\=\CYRI} + \e343{i macron}{\=\cyri} + \e344{I diaeresis}{\"\CYRI} + \e345{i diaeresis}{\"\cyri} + \e346{O diaeresis}{\"\CYRO} + \e347{o diaeresis}{\"\cyro} + \oct35 + \e350{barred O}\CYROTLD + \e351{barred o}\cyrotld + \e352{barred O diaeresis}{\"\CYROTLD} + \e353{barred o diaeresis}{\"\cyrotld} + \na354 + \na355 + \e356{U macron}{\=\CYRU} + \e357{u macron}{\=\cyru} + \oct36 + \e360{U diaeresis}{\"\CYRU} + \e361{u diaeresis}{\"\cyru} + \e362{U double acute}{\H\CYRU} + \e363{u double acute}{\H\cyru} + \e364{CHE diaeresis}{\"\CYRCH} + \e365{che diaeresis}{\"\cyrch} + \na366 + \na367 + \oct37 + \e370{YERU diaeresis}{\"\CYRERY} + \e371{yeru diaeresis}{\"\cyrery} + \na372 + \na373 + \na374 + \na375 + \na376 + \na377 +% + \tit040 + \oct00 + \na000 + \na001 + \na002 + \na003 + \na004 + \na005 + \na006 + \na007 + \oct01 + \na010 + \na011 + \na012 + \na013 + \na014 + \na015 + \na016 + \na017 + \oct02 + \na020 + \na021 + \na022 + \e023{en dash}\textendash + \e024{em dash}\textemdash + \na025 + \na026 + \na027 + \oct03 + \e030{left single quotation mark}\textquoteleft + \e031{right single quotation mark}\textquoteright + \e032{single low-9 quotation mark}\quotesinglbase + \na033 + \e034{left double quotation mark}\textquotedblleft + \alias\textgrqq + \alias\grqq + \e035{right double quotation mark}\textquotedblright + \e036{double low-9 quotation mark}\quotedblbase + \alias\textglqq + \alias\glqq + \na037 + \oct04 + \e040{dagger}\textdagger + \e041{double dagger}\textdaggerdbl + \e042{bullet}\textbullet + \na043 + \na044 + \na045 + \e046{horizontal ellipsis}\textellipsis + \na047 + \oct05 + \na050 + \na051 + \na052 + \na053 + \na054 + \na055 + \na056 + \na057 + \oct06 + \e060{per mille sign}\textperthousand + \e061{per ten thousand sign}\textpertenthousand + \na062 + \na063 + \na064 + \na065 + \na066 + \na067 + \oct07 + \na070 + \e071{single left-pointing angle quotation mark}\guilsinglleft + \e072{singe right-pointing angle quotation mark}\guilsinglright + \na073 + \na074 + \na075 + \na076 + \na077 + \oct10 + \na100 + \na101 + \na102 + \na103 + \e104{fraction slash}\textfractionsolidus + \na105 + \na106 + \na107 + \oct11 + \na110 + \na111 + \na112 + \na113 + \na114 + \na115 + \na116 + \na117 + \oct12 + \na120 + \na121 + \na122 + \na123 + \na124 + \na125 + \na126 + \na127 + \oct13 + \na130 + \na131 + \na132 + \na133 + \na134 + \na135 + \na136 + \na137 + \oct14 + \na140 + \na141 + \na142 + \na143 + \na144 + \na145 + \na146 + \na147 + \oct15 + \na150 + \na151 + \na152 + \na153 + \na154 + \na155 + \na156 + \na157 + \oct16 + \na160 + \na161 + \na162 + \na163 + \na164 + \na165 + \na166 + \na167 + \oct17 + \na170 + \na171 + \na172 + \na173 + \na174 + \na175 + \na176 + \na177 + \oct20 + \na200 + \na201 + \na202 + \na203 + \na204 + \na205 + \na206 + \na207 + \oct21 + \na210 + \na211 + \na212 + \na213 + \na214 + \na215 + \na216 + \na217 + \oct22 + \na220 + \na221 + \na222 + \na223 + \na224 + \na225 + \na226 + \na227 + \oct23 + \na230 + \na231 + \na232 + \na233 + \na234 + \na235 + \na236 + \na237 + \oct24 + \na240 + \na241 + \na242 + \na243 + \na244 + \na245 + \na246 + \na247 + \oct25 + \na250 + \na251 + \na252 + \na253 + \e254{Euro}\texteuro + \na255 + \na256 + \na257 + \oct26 + \na260 + \na261 + \na262 + \na263 + \na264 + \na265 + \na266 + \na267 + \oct27 + \na270 + \na271 + \na272 + \na273 + \na274 + \na275 + \na276 + \na277 + \oct30 + \na300 + \na301 + \na302 + \na303 + \na304 + \na305 + \na306 + \na307 + \oct31 + \na310 + \na311 + \na312 + \na313 + \na314 + \na315 + \na316 + \na317 + \oct32 + \na320 + \na321 + \na322 + \na323 + \na324 + \na325 + \na326 + \na327 + \oct33 + \na330 + \na331 + \na332 + \na333 + \na334 + \na335 + \na336 + \na337 + \oct34 + \na340 + \na341 + \na342 + \na343 + \na344 + \na345 + \na346 + \na347 + \oct35 + \na350 + \na351 + \na352 + \na353 + \na354 + \na355 + \na356 + \na357 + \oct36 + \na360 + \na361 + \na362 + \na363 + \na364 + \na365 + \na366 + \na367 + \oct37 + \na370 + \na371 + \na372 + \na373 + \na374 + \na375 + \na376 + \na377 +% + \tit041 + \symlist{\textcelsius\textnumero\texttrademark} + + \section*{\fileinfo} + Document: \textbf{\filename\space[\filedate\space\fileversion]} + \subsection*{Function} + This test file has several tasks: + \begin{itemize} + \item Testing package \emph{hyperref} with encoding file + \emph{puenc.def}. + \item Showing glyph commands and aliases that are supported by + package \emph{hyperref}. + \item Test for the pdf reader, especially \emph{AcrobatReader}. + Which glyphs of the \emph{Unicode} encoding are + correctly displayed? + \item These glyphs are shown that package \emph{hyperref} + replaces with simpler letters in order to avoid missing glyphs. + \end{itemize} + \subsection*{Short explanation of the bookmarks} + \begin{enumerate} + \item The outline entries of the first level show a summary of their + subentries. Second a screenshot with closed bookmarks + will contain all slots of the \emph{Unicode} encoding. + \item The second level of outline entries describes each slot or glyph: + \begin{enumerate} + \item \label{oct}% + Octal code of the slot in the \emph{Unicode} encoding. + \item The glyph is shown twice, surrounded by underscores: + The first one is produced by the octal sequence, see \ref{oct}. + The second one is the result of the higher glyph command, + see \ref{high}. + \item The glyph name of \emph{Unicode} encoding. + \item \label{high}% + The higher glyph \TeX-command, supported by + package \emph{hyperref}. + \end{enumerate} + \item Aliases of the glyph commands are shown as subentries of the + outline that describes the slot of that glyph command. + \end{enumerate} +\end{document} diff --git a/Master/texmf-dist/source/latex/hyperref/test/testbookmark.tex b/Master/texmf-dist/source/latex/hyperref/test/testbookmark.tex new file mode 100644 index 00000000000..bb6397061de --- /dev/null +++ b/Master/texmf-dist/source/latex/hyperref/test/testbookmark.tex @@ -0,0 +1,17 @@ +\documentclass[12pt]{article} +\usepackage{xspace} +\usepackage{hyperref} +\newcommand{\x}{x\xspace} + +\begin{document} + \section{Implicite space: \x world} + \section{Explicite spaces: \x\ world \x\space world \x~world} + \section{\x.+\x,+\x!+\x?+\x-+\x:+\x;+\x/+last-\x} + \makeatletter + \section{~|~~|~~~|~~~~|~~~~~|~~~~|~~~|~~|~} + \section{\x()(\x) } + \section{Italic correction: [\x\/]} + \section{::Nothing follows:} + \section{} + \section{\x} +\end{document} diff --git a/Master/texmf-dist/source/latex/hyperref/test/testfor2.tex b/Master/texmf-dist/source/latex/hyperref/test/testfor2.tex new file mode 100644 index 00000000000..d91596d5aad --- /dev/null +++ b/Master/texmf-dist/source/latex/hyperref/test/testfor2.tex @@ -0,0 +1,61 @@ +\documentclass{article} +\usepackage[dvips]{web} + +\def\r{\string\r} +\def\n{\string\n} + +\begin{document} +\begin{Form} + +\noindent First Sub total. + +\medskip\noindent +\makebox[.75in][l]{Number 1:} \TextField[width=1in,name=firstnum, +keystroke={AFNumber_Keystroke(2,0,0,0,"",true);}, +format={AFNumber_Format(2,0,0,0,"",true);}]{} + +\medskip\noindent +\makebox[.75in][l]{Number 2:} \TextField[width=1in,name=secondnum, +keystroke={AFNumber_Keystroke(2,0,0,0,"",true);}, +format={AFNumber_Format(2,0,0,0,"",true);}]{} + +\medskip\noindent +\makebox[.75in][l]{Sub total:} \TextField[width=1in,name=total1,align={0 /_objdef {total1}}, +format={AFNumber_Format(2,0,0,0,"",true);}, keystroke={AFNumber_Keystroke(2,0,0,0,"",true);}, +calculate={AFSimple_Calculate("SUM",new Array("firstnum", "secondnum"));\string\040}, +format={AFNumber_Format(2,0,0,0,"",true);}]{} + +\bigskip\noindent Second Sub total: + +\medskip\noindent +\makebox[.75in][l]{Number 1:} \TextField[width=1in,name=Number.1, +keystroke={AFNumber_Keystroke(2,0,0,0,"",true);}, +format={AFNumber_Format(2,0,0,0,"",true);}]{} + +\medskip\noindent +\makebox[.75in][l]{Number 2:} \TextField[width=1in,name=Number.2, +keystroke={AFNumber_Keystroke(2,0,0,0,"",true);}, +format={AFNumber_Format(2,0,0,0,"",true);}]{} + +\medskip\noindent +\makebox[.75in][l]{Total:} \TextField[width=1in,name=total2, +format={AFNumber_Format(2,0,0,0,"",true);},align={0 /_objdef {total2}}, +keystroke={AFNumber_Keystroke(2,0,0,0,"",true);}, +calculate={AFSimple_Calculate("SUM",new Array("Number"));\r}, +format={AFNumber_Format(2,0,0,0,"",true);}]{} + + + +\bigskip\noindent +\makebox[.75in][l]{Grand Total:} \TextField[width=1in,name=total, +format={AFNumber_Format(2,0,0,0,"",true);},align={0 /_objdef {total}}, +keystroke={AFNumber_Keystroke(2,0,0,0,"",true);}, +calculate={this.getField("total").value=this.getField("total1").value+% + this.getField("total2").value;\r}, +format={AFNumber_Format(2,0,0,0,"",true);}]{} + + +\special{! [ {corder} 0 [ {total1} {total2} {total} ] /PUTINTERVAL pdfmark} + +\end{Form} +\end{document} diff --git a/Master/texmf-dist/source/latex/hyperref/test/testform.tex b/Master/texmf-dist/source/latex/hyperref/test/testform.tex new file mode 100644 index 00000000000..8ddc3f7d9b9 --- /dev/null +++ b/Master/texmf-dist/source/latex/hyperref/test/testform.tex @@ -0,0 +1,50 @@ +%\begin{Form}[action=http:www.rhbnc.ac.uk/htbin/shew-fields,html,method=post] + +\documentclass{article} +\usepackage[bookmarks=false]{hyperref} +\setlength{\parindent}{0pt} +\setlength{\parskip}{10pt} +\begin{document} +\begin{Form}[action=mailto:srahtz,encoding=html,method=post] + +\TextField[width=3in,name=xname,value={Bilbo Baggins}] + {Full name: } + +%\TextField[name=warfs,validate={AFRange_Validate\string\(true, 1, true, 13\string\);}] +% {How many dwarves came along: } + +\TextField[multiline,width=1in,name=address,borderstyle=D, + color=1 1 1,backgroundcolor=0 0 .5, + value={Bag End, The Hill, Hobbiton}]{Address: } + +\ChoiceMenu[default=Home,menulength=3,width=2in,name=travel,default=Beorn] + {Favorite part of your travels:} + {Trolls,Misty Mountains,Beorn,Mirkwood,Elves,Laketown,% + Smaug,The Battle} + +Have you still got your: +\CheckBox[]{Sword} +\CheckBox[name=coat]{Mithril coat} +%\CheckBox[name=ring,checked]{\textbf{Ring!}} +\CheckBox[name=ring,checked]{Ring!} + +\ChoiceMenu[radio,default=Again,name=next,borderwidth=3,bordercolor=0 1 0] + {Do you want to:} + {Do it all again=Again, + Pretend it never happened=Forget, + Write a book about it=Write} + +%\TextField[password,name=made]{\emph{Who} made the ring? } +\TextField[password,name=made]{Who made the ring? } + +\ChoiceMenu[combo,default=Bofur,name=whatdwarf, + ]{Select funniest name, or add one} + {Bofur,Thorin,Gollum,Smaug,Gandalf} + +%\PushButton[name=xxx,onclick={app.beep(0)}]{Make a horrid beep} + +\Submit{Send} +\Reset{Clear} + +\end{Form} +\end{document} diff --git a/Master/texmf-dist/source/latex/hyperref/test/testnb.tex b/Master/texmf-dist/source/latex/hyperref/test/testnb.tex new file mode 100644 index 00000000000..42abd8e0ac6 --- /dev/null +++ b/Master/texmf-dist/source/latex/hyperref/test/testnb.tex @@ -0,0 +1,50 @@ +\documentclass{article} +\usepackage[german]{babel} +\usepackage[numbers,sort&compress]{natbib} +\usepackage{hyperref} +\usepackage{times} + +\begin{document} + +In addition, this theory---that of the German sociologist Niklas +Luhmann---is one +of the most (if not the most) powerful +contemporary general sociological theories +\citep{luhm:DoS,Luhm:Soc&int,luhm:WrtdG}. Therefore, in the rest of +this section, rather than making an eclectic use of different social +theories, I briefly present portions of Luhmann's theory. + +\begin{thebibliography}{3} +\expandafter\ifx\csname natexlab\endcsname\relax\def\natexlab#1{#1}\fi + +\bibitem[Luhmann(1982)]{luhm:DoS} +Niklas Luhmann. +\newblock {\em The Differentiation of Society}. +\newblock New York: Columbia University Press, 1982. + +\bibitem[Luhmann(1987)]{Luhm:Soc&int} +Niklas Luhmann. +\newblock The evolutionary differentiation between society and interaction. +\newblock In Jeffrey~C. Alexander, Bernhard Giesen, Richard Muench, and Neil~J. + Smelser, editors, {\em The Micro-Macro Link}, pages 112--31. Berkeley: + University of California Press, 1987. + +\bibitem[Luhmann(1988)]{luhm:WrtdG} +Niklas Luhmann. +\newblock {\em Die Wirtschaft der Gesellschaft}. +\newblock Frankfurt am Main: Suhrkamp, 1988. + +\end{thebibliography} +\end{document} +\usepackage +[%linkcolor=yellow, + citecolor=yellow, + citebordercolor={.5 .5 0}, + pdftitle={Testing natbib and hyperref}, + pdfauthor={SPQR and PWD}, + pdfsubject={Dummy stuff}, + pdfkeywords=Luhmann, +% pdfstartview=/FitB, + pdfpagemode=UseThumbs +] +{hyperref} diff --git a/Master/texmf-dist/source/latex/hyperref/test/testoz.tex b/Master/texmf-dist/source/latex/hyperref/test/testoz.tex new file mode 100644 index 00000000000..f56c111a976 --- /dev/null +++ b/Master/texmf-dist/source/latex/hyperref/test/testoz.tex @@ -0,0 +1,38 @@ +\documentclass{article} +\usepackage{hyperref} +\begin{document} +\section{Pointing to dvi names} +\href{dvi::TeX-docs:nasty.dvi}{relative path to nasty.dvi}!\par +\href{:TeX-docs:nasty.dvi}{relative path to nasty.dvi}!\par +\href{HD:OzTeX:TeX-docs:nasty.dvi}{full path to nasty.dvi}!\par +\href{dvi:HD:OzTeX:TeX-docs:nasty.dvi}{full path to nasty.dvi}!\par +\href{dvi:nasty.dvi}{nasty.dvi in current folder}!\par +\href{dvi:nasty.dvi@3}{page 3 in nasty.dvi}!\par +\href{nasty.dvi@3}{page 3 in nasty.dvi}!\par +\href{nasty.dvi}{nasty.dvi}!\par +\href{file:nasty.dvi}{nasty.dvi}!\par +\href{file:HD:OzTeX:TeX-docs:nasty.dvi}{full path to nasty.dvi}!\par +\href{dvi:ozuser.dvi#section.12}{section 12 in user guide}!\par + +\href{x/y/z.dvi}{x/y/z.dvi} +\href{/x/y/z.dvi}{/x/y/z.dvi} +\href{http://x/y/z.dvi}{http://x/y/z.dvi} +\href{http://x:80/y/z.dvi}{http://x:80/y/z.dvi} +\section{Pointing to pdf names} +\href{dvi::TeX-docs:nasty.pdf}{relative path to nasty.pdf}!\par +\href{:TeX-docs:nasty.pdf}{relative path to nasty.pdf}!\par +\href{HD:OzTeX:TeX-docs:nasty.pdf}{full path to nasty.pdf}!\par +\href{dvi:HD:OzTeX:TeX-docs:nasty.pdf}{full path to nasty.pdf}!\par +\href{dvi:nasty.pdf}{nasty.pdf in current folder}!\par +\href{dvi:nasty.pdf@3}{page 3 in nasty.pdf}!\par +\href{nasty.pdf@3}{page 3 in nasty.pdf}!\par +\href{nasty.pdf}{nasty.pdf}!\par +\href{file:nasty.pdf}{nasty.pdf}!\par +\href{file:HD:OzTeX:TeX-docs:nasty.pdf}{full path to nasty.pdf}!\par +\href{dvi:ozuser.pdf#section.12}{section 12 in user guide}!\par + +\href{x/y/z.pdf}{x/y/z.pdf} +\href{/x/y/z.pdf}{/x/y/z.pdf} +\href{http://x/y/z.pdf}{http://x/y/z.pdf} +\href{http://x:80/y/z.pdf}{http://x:80/y/z.pdf} +\end{document} diff --git a/Master/texmf-dist/source/latex/hyperref/test/testslide.tex b/Master/texmf-dist/source/latex/hyperref/test/testslide.tex new file mode 100644 index 00000000000..fa367b556a2 --- /dev/null +++ b/Master/texmf-dist/source/latex/hyperref/test/testslide.tex @@ -0,0 +1,101 @@ +% dummy file seminar.con, if it does not exist. +\begin{filecontents}{seminar.con} +\end{filecontents} +\documentclass[]{seminar} +\usepackage{slidesec} +\def\thepage{E\arabic{page}} +\usepackage{lastpage} +\usepackage{xspace} +\usepackage{makeidx} +\usepackage[pdfstartview={FitBH -32768},pdfpagemode=None,plainpages=false,colorlinks]{hyperref} +\hypersetup{pdfauthor=?`\c C\"asar M\"uller n\~ao!`} +\setcounter{tocdepth}{4} +\setcounter{secnumdepth}{4} +\makeindex +\hypersetup{pdftitle=Welcome to the Monkey House} +\newcommand{\ANS}{\textsf{ANSYS}\xspace} +\begin{document} +\begin{slide} +\slideheading{xx} +\end{slide} +\begin{slide} +\listofslides +\end{slide} + +\begin{slide} +\slideheading{A funny \ANS-section} +Page 1; See \textcolor{red}{page} --\pageref{page2}-- +\end{slide} +\begin{slide} +Page 2; this is page 2\label{page2} +\end{slide} + +\begin{slide} +\index{an item on slide 3} + +\htmladdnormallink{A dummy URL}{http://www.tug.org/A-Fake_URL.html} + +\Acrobatmenu{Quit}{End Acrobat Reader} + +\Acrobatmenu{FullScreen}{Switch to full screen} + +\Acrobatmenu{ZoomIn}{Zoom in} + +$\int\!dx$ +\end{slide} +\begin{slide} +\slideheading{Yet another ?`\c C\"asar M\"uller n\~ao!`} + +\end{slide} +\begin{slide} +\slideheading{Testing Int\'ernal J\oe mps}\label{ss:intjmps} + +This is some text and this is a \hypertarget{target}{target}. + +\end{slide} +\begin{slide} +Now lets jump to \hyperlink{target}{Target}. + +Let's try going to Section~\ref{ss:intjmps} + +\end{slide} +\begin{slide} +\slideheading{A \ss ection with $\leq$} +xx +xx +\subsubsection{A subsubsection \texorpdfstring{$a+b$}{a+b}} +xx +\paragraph{A paragraph} +xx +\subparagraph{A subparagraph} +xxx +\end{slide} +\begin{slide} +\slideheading{Testing External Jumps}\label{ss:extjmps} + +\begin{enumerate} + +\item Jump to an external: The jump +\href{file:test7#TestTarget}{target} should open test7.pdf on +page 2, +\item Jump to an external: The jump +\href{file:test7#page.1}{page 1} should open test7.pdf on +page 1. + +%\item Jump to an relative external strange file +%\href{/D/srahtz/skills.doc}{destination} + +\href{run:picture.eps}{a PS file to launch} + +\href{run:fontman.exe}{an application} + +\href{run:e:\string\\mdraw\string\\mdraw.exe#picture.eps}{a PS file to launch (2)} +\end{enumerate} +\end{slide} +\begin{slide} +\printindex +\end{slide} +\end{document} + + + diff --git a/Master/texmf-dist/source/latex/hyperref/test/testurl.bbl b/Master/texmf-dist/source/latex/hyperref/test/testurl.bbl new file mode 100644 index 00000000000..b9a3697a343 --- /dev/null +++ b/Master/texmf-dist/source/latex/hyperref/test/testurl.bbl @@ -0,0 +1,8 @@ +\begin{thebibliography}{1} + +\bibitem{THE} +David~Loberg Code. +\newblock Aural comprehension guide (webpage). +\newblock \url{http://www.wmich.edu/mus-theo/etg/et_guide.html}. + +\end{thebibliography} diff --git a/Master/texmf-dist/source/latex/hyperref/test/testurl.bib b/Master/texmf-dist/source/latex/hyperref/test/testurl.bib new file mode 100644 index 00000000000..883c938fa1c --- /dev/null +++ b/Master/texmf-dist/source/latex/hyperref/test/testurl.bib @@ -0,0 +1,6 @@ +@MISC{THE, + key={the}, + author={David Loberg Code}, + title={Aural Comprehension Guide (Webpage)}, + note={\url{http://www.wmich.edu/mus-theo/etg/et_guide.html}} +} diff --git a/Master/texmf-dist/source/latex/hyperref/test/testurl.tex b/Master/texmf-dist/source/latex/hyperref/test/testurl.tex new file mode 100644 index 00000000000..d2a2a6f0b6d --- /dev/null +++ b/Master/texmf-dist/source/latex/hyperref/test/testurl.tex @@ -0,0 +1,14 @@ +\documentclass[11pt]{article} +\usepackage[]{color} +\usepackage[letterpaper,colorlinks,breaklinks,backref]{hyperref} +%\usepackage{url} %use as alternative to hyperref for testing +\newcommand{\myurl}[1]{{\url{{#1}}}} + +\begin{document} +\url{http://www.wmich.edu/mus-theo/etg/et_guide.html} %ok now with hyperref, ok with url +\myurl{http://www.wmich.edu/mus-theo/etg/et_guide.html} %fails with hyperref, ok with url + +\cite{THE} +\bibliographystyle{unsrt} +\bibliography{testurl}%fails with hyperref, ok with url +\end{document} |