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+++ b/support/hypertex/tanmoy/examples/Anomalkap.aux
@@ -0,0 +1,123 @@
+\relax
+\citation{KP}
+\citation{Jan}
+\citation{CS}
+\citation{KP}
+\citation{FS}
+\citation{Neu}
+\citation{Neu2}
+\citation{AK}
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+\newlabel{sec:int}{{\relax \let \hyper@@@ \relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{section}{\uppercase {i}}{\uppercase {i}}}{3}}
+\citation{KP}
+\citation{Alt}
+\citation{Dis}
+\citation{CS}
+\citation{Neu}
+\citation{Neu}
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+\citation{chiral}
+\citation{Neu}
+\@writefile{toc}{\string\contentsline\space {section}{\string\numberline\space {\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{section}{\uppercase {ii}}{\hbox {\hskip 1pt\relax \uppercase {ii}}}\hskip -1pt\relax }Action, Fermion Propagator and Chiral Zero Modes}{5}}
+\newlabel{sec:model}{{\relax \let \hyper@@@ \relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{section}{\uppercase {ii}}{\uppercase {ii}}}{5}}
+\@writefile{toc}{\string\contentsline\space {subsection}{\string\numberline\space {\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{subsection}{A}{\hbox {\hskip 1pt\relax A}}\hskip -1pt\relax }Lattice Action}{5}}
+\citation{Neu}
+\citation{KP}
+\citation{Neu}
+\citation{Dis}
+\citation{Neu}
+\citation{Neu}
+\citation{Alt}
+\newlabel{actionf}{{\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{equation}{3}{3}}{6}}
+\citation{Neu}
+\citation{CS}
+\@writefile{toc}{\string\contentsline\space {subsection}{\string\numberline\space {\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{subsection}{B}{\hbox {\hskip 1pt\relax B}}\hskip -1pt\relax }Chiral Zero Modes}{7}}
+\citation{Neu}
+\@writefile{toc}{\string\contentsline\space {subsection}{\string\numberline\space {\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{subsection}{C}{\hbox {\hskip 1pt\relax C}}\hskip -1pt\relax }Fermion Propagator and Zero Modes}{8}}
+\newlabel{fprop}{{\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{equation}{11}{11}}{8}}
+\newlabel{gl}{{\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{equation}{13}{13}}{8}}
+\citation{Neu}
+\citation{Neu}
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+\newlabel{gr}{{\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{equation}{14}{14}}{9}}
+\citation{Sham}
+\citation{Sham}
+\citation{Dis}
+\newlabel{wil}{{\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{equation}{17}{17}}{10}}
+\newlabel{shl}{{\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{equation}{18}{18}}{10}}
+\newlabel{shr}{{\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{equation}{19}{19}}{10}}
+\@writefile{toc}{\string\contentsline\space {subsection}{\string\numberline\space {\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{subsection}{D}{\hbox {\hskip 1pt\relax D}}\hskip -1pt\relax }Fermion Feynman Rules }{10}}
+\@writefile{toc}{\string\contentsline\space {section}{\string\numberline\space {\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{section}{\uppercase {iii}}{\hbox {\hskip 1pt\relax \uppercase {iii}}}\hskip -1pt\relax }Perturbative Calculations for the Chiral Schwinger Model}{11}}
+\newlabel{sec:2dim}{{\relax \let \hyper@@@ \relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{section}{\uppercase {iii}}{\uppercase {iii}}}{11}}
+\@writefile{toc}{\string\contentsline\space {subsection}{\string\numberline\space {\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{subsection}{A@}{\hbox {\hskip 1pt\relax A}}\hskip -1pt\relax }Effective Action at Fermion One-Loop}{12}}
+\@writefile{toc}{\string\contentsline\space {subsection}{\string\numberline\space {\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{subsection}{B@}{\hbox {\hskip 1pt\relax B}}\hskip -1pt\relax }Evaluation of Zero Mode Contributions}{12}}
+\citation{Dis}
+\newlabel{sumf}{{\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{equation}{37}{37}}{14}}
+\@writefile{toc}{\string\contentsline\space {subsection}{\string\numberline\space {\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{subsection}{C@}{\hbox {\hskip 1pt\relax C}}\hskip -1pt\relax }Evaluation of Remaining Contributions}{14}}
+\newlabel{gcs}{{\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{equation}{39}{39}}{14}}
+\citation{CS}
+\citation{CS}
+\newlabel{sum}{{\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{equation}{41}{41}}{15}}
+\newlabel{cst}{{\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{equation}{42}{42}}{15}}
+\citation{FS}
+\citation{Neu,AK}
+\citation{chiral}
+\citation{Dis}
+\citation{chiral}
+\newlabel{sumk}{{\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{equation}{44}{44}}{16}}
+\@writefile{toc}{\string\contentsline\space {subsection}{\string\numberline\space {\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{subsection}{D@}{\hbox {\hskip 1pt\relax D}}\hskip -1pt\relax }Total Contributions}{16}}
+\newlabel{eff}{{\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{equation}{45}{45}}{16}}
+\citation{Neu}
+\citation{Neu2}
+\citation{JR}
+\@writefile{toc}{\string\contentsline\space {section}{\string\numberline\space {\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{section}{\uppercase {iv}}{\hbox {\hskip 1pt\relax \uppercase {iv}}}\hskip -1pt\relax }Anomalies in the Chiral Schwinger Model}{17}}
+\newlabel{sec:anomaly}{{\relax \let \hyper@@@ \relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{section}{\uppercase {iv}}{\uppercase {iv}}}{17}}
+\@writefile{toc}{\string\contentsline\space {subsection}{\string\numberline\space {\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{subsection}{A@@}{\hbox {\hskip 1pt\relax A}}\hskip -1pt\relax }Currents and their Divergence}{17}}
+\newlabel{current}{{\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{equation}{49}{49}}{18}}
+\@writefile{toc}{\string\contentsline\space {subsection}{\string\numberline\space {\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{subsection}{B@@}{\hbox {\hskip 1pt\relax B}}\hskip -1pt\relax }Gauge invariance}{18}}
+\newlabel{sum0a}{{\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{equation}{52}{52}}{18}}
+\citation{Jan}
+\newlabel{sum0b}{{\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{equation}{53}{53}}{19}}
+\@writefile{toc}{\string\contentsline\space {subsection}{\string\numberline\space {\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{subsection}{C@@}{\hbox {\hskip 1pt\relax C}}\hskip -1pt\relax }Gauge Anomalies}{19}}
+\citation{KP,CS}
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+\@writefile{toc}{\string\contentsline\space {subsection}{\string\numberline\space {\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{subsection}{D@@}{\hbox {\hskip 1pt\relax D}}\hskip -1pt\relax }Chern-Simons Current}{20}}
+\citation{CS}
+\citation{Dis}
+\citation{KP,Jan,Dis}
+\citation{Dis}
+\@writefile{toc}{\string\contentsline\space {subsection}{\string\numberline\space {\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{subsection}{E}{\hbox {\hskip 1pt\relax E}}\hskip -1pt\relax }Pythagorean Chiral Schwinger Model and Anomaly in Fermion Number Current}{21}}
+\citation{Dis}
+\citation{Neu}
+\citation{AK}
+\citation{Dis}
+\citation{chiral}
+\@writefile{toc}{\string\contentsline\space {section}{\string\numberline\space {\relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{section}{\uppercase {v}}{\hbox {\hskip 1pt\relax \uppercase {v}}}\hskip -1pt\relax }conclusions}{23}}
+\newlabel{sec:concl}{{\relax \let \hyper@@@ \relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{section}{\uppercase {v}}{\uppercase {v}}}{23}}
+\citation{Neu}
+\citation{Neu3}
+\citation{Neu2}
+\bibcite{KP}{1}
+\bibcite{Jan}{2}
+\bibcite{CS}{3}
+\bibcite{FS}{4}
+\bibcite{Neu}{5}
+\bibcite{Neu2}{6}
+\bibcite{AK}{7}
+\bibcite{Alt}{8}
+\bibcite{Dis}{9}
+\bibcite{Sham}{10}
+\bibcite{chiral}{11}
+\bibcite{JR}{12}
+\bibcite{Neu3}{13}
+\@writefile{lof}{\string\contentsline\space {figure}{\string\numberline\space {1}{\ignorespaces Two zero modes $u_L$ and $u_R$ as a function of $s$ at $m_0=0.1$ and 0.5 for $p_1=p_2=0$. We take $L=100$.}}{26}}
+\newlabel{zero}{{\relax \let \hyper@@@ \relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{figure}{1}{1}}{26}}
+\@writefile{lof}{\string\contentsline\space {figure}{\string\numberline\space {2}{\ignorespaces The coefficient of the anomaly $C(s)$ for the Kaplan's method as a function of $s$ at $m_0=0.1$ and 0.5 for $L=100$.}}{26}}
+\newlabel{anomalyK}{{\relax \let \hyper@@@ \relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{figure}{2}{2}}{26}}
+\@writefile{lof}{\string\contentsline\space {figure}{\string\numberline\space {3}{\ignorespaces The coefficient of the anomaly $C(s)$ for the Shamir's method as a function of $s$ at $m_0=0.1$ and 0.5 for $L=100$.}}{26}}
+\newlabel{anomalyS}{{\relax \let \hyper@@@ \relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{figure}{3}{3}}{26}}
+\@writefile{lof}{\string\contentsline\space {figure}{\string\numberline\space {4}{\ignorespaces The coefficient of the Chern-Simons current $I(s)$ for the Kaplan's method as a function of $s$ at $m_0=0.1$ and 0.5 for $L=100$.}}{26}}
+\newlabel{CSK}{{\relax \let \hyper@@@ \relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{figure}{4}{4}}{26}}
+\@writefile{lof}{\string\contentsline\space {figure}{\string\numberline\space {5}{\ignorespaces The coefficient of the Chern-Simons current $I(s)$ for the Shamir's method as a function of $s$ at $m_0=0.1$ and 0.5 for $L=100$.}}{26}}
+\newlabel{CSS}{{\relax \let \hyper@@@ \relax \let \hyper@@@ \relax \let \hyper@@@ \hyper@ \hyperpr@ref {}{figure}{5}{5}}{26}}