Convert generic LaTeX files to NTCIR compatible HTML

To generate NTCIR compatible (X)HTML output we need to be able to generate the NTCIR file output from the TeX sources. As preliminary task I was trying to reproduce the conversion of https://arxiv.org/format/1305.2869v1 Therefore two steps are required

convert tex2xml

latexml --includestyles src/dws.tex --destination=tex.xml

convert xml2xhtml

ubuntu@master:/data2/mathpd/texfiles/playground/1305.2869$ latexmlpost --format xhtml --cmml --pmml --mathtex --destination=./out/out --splitnaming=id --splitpath="//ltx:section | //ltx:subsection | //ltx:bibliography | //ltx:appendix | //ltx:index |//ltx:para" --navigationtoc=none --dbfile=db.bd --nopictureimages --nographicimages tex.xml

However there are still some differences between the converted files

file names

ls refs/
1305.2869_1_10.xhtml  1305.2869_1_15.xhtml  1305.2869_1_1.xhtml   1305.2869_1_24.xhtml  1305.2869_1_29.xhtml  1305.2869_1_33.xhtml  1305.2869_1_5.xhtml
1305.2869_1_11.xhtml  1305.2869_1_16.xhtml  1305.2869_1_20.xhtml  1305.2869_1_25.xhtml  1305.2869_1_2.xhtml   1305.2869_1_34.xhtml  1305.2869_1_6.xhtml
1305.2869_1_12.xhtml  1305.2869_1_17.xhtml  1305.2869_1_21.xhtml  1305.2869_1_26.xhtml  1305.2869_1_30.xhtml  1305.2869_1_35.xhtml  1305.2869_1_7.xhtml
1305.2869_1_13.xhtml  1305.2869_1_18.xhtml  1305.2869_1_22.xhtml  1305.2869_1_27.xhtml  1305.2869_1_31.xhtml  1305.2869_1_3.xhtml   1305.2869_1_8.xhtml
1305.2869_1_14.xhtml  1305.2869_1_19.xhtml  1305.2869_1_23.xhtml  1305.2869_1_28.xhtml  1305.2869_1_32.xhtml  1305.2869_1_4.xhtml   1305.2869_1_9.xhtml

ls out/
bib            ltx-article.css  S1.p1  S1.p4  S2.p10  S2.p13  S2.p16  S2.p3  S2.p6  S2.p9  S3.p10  S3.p4  S3.p7  S4     S4.p3  Sx1.p1
LaTeXML.cache  out              S1.p2  S2     S2.p11  S2.p14  S2.p17  S2.p4  S2.p7  S3     S3.p2   S3.p5  S3.p8  S4.p1  src
LaTeXML.css    S1               S1.p3  S2.p1  S2.p12  S2.p15  S2.p2   S2.p5  S2.p8  S3.p1  S3.p3   S3.p6  S3.p9  S4.p2  Sx1

file contents

cat out/S1.p1
<?xml version="1.0" encoding="utf-8"?>
<!DOCTYPE html PUBLIC "-//W3C//DTD XHTML 1.1 plus MathML 2.0//EN" "http://www.w3.org/Math/DTD/mathml2/xhtml-math11-f.dtd">
<html xmlns="http://www.w3.org/1999/xhtml">
<head>
<title>Untitled Document</title>
<!--Generated on Wed Nov 30 10:24:24 2016 by LaTeXML (version 0.8.1) http://dlmf.nist.gov/LaTeXML/.-->
<!--Document created on May 2013.-->

<meta http-equiv="Content-Type" content="application/xhtml+xml; charset=UTF-8"/>
<link rel="stylesheet" href="LaTeXML.css" type="text/css"/>
<link rel="stylesheet" href="ltx-article.css" type="text/css"/>
<link rel="up" href="S1" title="1 Introduction ‣ DCPT-13/17 The dynamics of domain wall Skyrmions"/>
<link rel="up up" href="out" title="DCPT-13/17 The dynamics of domain wall Skyrmions"/>
<link rel="start" href="out" title="DCPT-13/17 The dynamics of domain wall Skyrmions"/>
<link rel="prev" href="S1" title="1 Introduction ‣ DCPT-13/17 The dynamics of domain wall Skyrmions"/>
<link rel="next" href="S2" title="2 The model and its static Skyrmion ‣ DCPT-13/17 The dynamics of domain wall Skyrmions"/>
<link rel="sidebar" href="S1.p2" title="1 Introduction ‣ DCPT-13/17 The dynamics of domain wall Skyrmions"/>
<link rel="sidebar" href="S1.p3" title="1 Introduction ‣ DCPT-13/17 The dynamics of domain wall Skyrmions"/>
<link rel="sidebar" href="S1.p4" title="1 Introduction ‣ DCPT-13/17 The dynamics of domain wall Skyrmions"/>
<link rel="section" href="S1" title="1 Introduction ‣ DCPT-13/17 The dynamics of domain wall Skyrmions"/>
<link rel="section" href="S2" title="2 The model and its static Skyrmion ‣ DCPT-13/17 The dynamics of domain wall Skyrmions"/>
<link rel="section" href="S3" title="3 Skyrmion dynamics ‣ DCPT-13/17 The dynamics of domain wall Skyrmions"/>
<link rel="section" href="S4" title="4 Conclusion ‣ DCPT-13/17 The dynamics of domain wall Skyrmions"/>
<link rel="section" href="Sx1" title="Acknowledgements ‣ DCPT-13/17 The dynamics of domain wall Skyrmions"/>
<link rel="bibliography" href="bib" title="References ‣ DCPT-13/17 The dynamics of domain wall Skyrmions"/>
</head>
<body>
<div class="ltx_page_main">
<div class="ltx_page_header">
<div><a href="S1" title="1 Introduction ‣ DCPT-13/17 The dynamics of domain wall Skyrmions" class="ltx_ref" rel="up"><span class="ltx_text ltx_ref_title"><span class="ltx_tag ltx_tag_ref">1 </span>Introduction</span></a><a href="S1" title="1 Introduction ‣ DCPT-13/17 The dynamics of domain wall Skyrmions" class="ltx_ref" rel="prev"><span class="ltx_text ltx_ref_title"><span class="ltx_tag ltx_tag_ref">1 </span>Introduction</span></a><a href="S2" title="2 The model and its static Skyrmion ‣ DCPT-13/17 The dynamics of domain wall Skyrmions" class="ltx_ref" rel="next"><span class="ltx_text ltx_ref_title"><span class="ltx_tag ltx_tag_ref">2 </span>The model and its static Skyrmion</span></a>
</div></div>
<div class="ltx_page_content">
<div class="ltx_para ltx_authors_1line">
<p class="ltx_p">Skyrmions <cite class="ltx_cite ltx_citemacro_cite">[<a href="bib#bib1" title="" class="ltx_ref">1</a>]</cite> are topological solitons in
generalized sigma models that include a term in the Lagrangian that is
quartic in the derivatives of the field.
The role of this quartic Skyrme term is to provide a fixed finite size for
the Skyrmion, as revealed by Derrick’s theorem <cite class="ltx_cite ltx_citemacro_cite">[<a href="bib#bib2" title="" class="ltx_ref">2</a>]</cite>.
The original Skyrme model is a relativistic theory in (3+1)-dimensions,
where Skyrmions describe baryons within an effective field theory.
There is also a (2+1)-dimensional analogue of this theory,
known as the baby Skyrme model <cite class="ltx_cite ltx_citemacro_cite">[<a href="bib#bib3" title="" class="ltx_ref">3</a>]</cite>. This is a generalization of the
O(3) sigma model, and has proved to be a useful
testing ground for the study of several aspects of Skyrmions.</p>
</div>
</div>
<div class="ltx_page_footer">
<div><a href="S1" title="1 Introduction ‣ DCPT-13/17 The dynamics of domain wall Skyrmions" class="ltx_ref" rel="prev"><span class="ltx_text ltx_ref_title"><span class="ltx_tag ltx_tag_ref">1 </span>Introduction</span></a><a href="bib" title="References ‣ DCPT-13/17 The dynamics of domain wall Skyrmions" class="ltx_ref" rel="bibliography"><span class="ltx_text ltx_ref_title">References</span></a><a href="S2" title="2 The model and its static Skyrmion ‣ DCPT-13/17 The dynamics of domain wall Skyrmions" class="ltx_ref" rel="next"><span class="ltx_text ltx_ref_title"><span class="ltx_tag ltx_tag_ref">2 </span>The model and its static Skyrmion</span></a>
</div>
<div class="ltx_page_logo">Generated  on Wed Nov 30 10:24:24 2016 by <a href="http://dlmf.nist.gov/LaTeXML/">LaTeXML <img src="data:image/png;base64,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" alt="[LOGO]"/></a></div></div>
</div>
</body>
</html>

vs.

cat refs/1305.2869_1_1.xhtml
<?xml version="1.0" encoding="utf-8"?>
<html xmlns="http://www.w3.org/1999/xhtml">
<head>
<meta http-equiv="Content-Type" content="application/xhtml+xml; charset=UTF-8" /></head><body>
<div class="ltx_para" id="S1.p1">
<p class="ltx_p" id="S1.p1.1">Skyrmions <cite class="ltx_cite">[<a href="#bib.bib1" class="ltx_ref" title="">1</a>]</cite> are topological solitons in
generalized sigma models that include a term in the Lagrangian that is
quartic in the derivatives of the field.
The role of this quartic Skyrme term is to provide a fixed finite size for
the Skyrmion, as revealed by Derrick’s theorem <cite class="ltx_cite">[<a href="#bib.bib2" class="ltx_ref" title="">2</a>]</cite>.
The original Skyrme model is a relativistic theory in (3+1)-dimensions,
where Skyrmions describe baryons within an effective field theory.
There is also a (2+1)-dimensional analogue of this theory,
known as the baby Skyrme model <cite class="ltx_cite">[<a href="#bib.bib3" class="ltx_ref" title="">3</a>]</cite>. This is a generalization of the
O(3) sigma model, and has proved to be a useful
testing ground for the study of several aspects of Skyrmions.</p>
</div>
</body></html>

gipplab / mathosphere

Convert generic LaTeX files to NTCIR compatible HTML #122

file names

file contents