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\@writefile{lof}{\contentsline {figure}{\numberline {1}{\ignorespaces \it  The KTeV detector.  }}{3}}
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\@writefile{toc}{\contentsline {section}{\numberline {2}$K_L\to \pi ^0\nu \mathaccent "7016\relax \nu $}{3}}
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\@writefile{lof}{\contentsline {figure}{\numberline {2}{\ignorespaces \it  The reconstructed transverse momentum for $K_L\to \pi ^0\nu \mathaccent "7016\relax \nu $ candidates. The solid histogram represents the sum of our Monte Carlo background estimate. No candidates are found in the signal region indicated in the figure.  }}{4}}
\newlabel{fig:pznn}{{2}{4}}
\citation{piee_paper}
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\@writefile{toc}{\contentsline {section}{\numberline {3}$K_L\to \pi ^0e^+e^-$}{5}}
\@writefile{toc}{\contentsline {section}{\numberline {4}$K_L\to \pi ^0\mu ^+\mu ^-$}{5}}
\@writefile{lof}{\contentsline {figure}{\numberline {3}{\ignorespaces \it  Reconstructed $\gamma \gamma $ mass versus $e^+e^-\gamma \gamma $ mass for $K_L\to \pi ^0e^+e^-$ candidates. The square region represents the area masked off while the selection criteria were determined. The ellipse represents the signal region. One candidate event is present in the signal region.  }}{6}}
\newlabel{fig:pzee}{{3}{6}}
\@writefile{toc}{\contentsline {section}{\numberline {5}Summary and Conclusions}{6}}
\bibcite{new_phys}{1}
\bibcite{na48_pi0ee}{2}
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\bibcite{na48_pi0gg}{4}
\bibcite{ktev_pi0gg}{5}
\@writefile{lof}{\contentsline {figure}{\numberline {4}{\ignorespaces \it  The reconstructed $\mu ^+\mu ^-\gamma \gamma $ mass for $K_L\to \pi ^0\mu ^+\mu ^-$ candidates. The solid histogram represents a Monte Carlo prediction of our estimated background. Two events were found in the signal region indicated by the arrows.  }}{7}}
\newlabel{fig:pzmm}{{4}{7}}
\bibcite{buras}{6}
\bibcite{isidori}{7}
\bibcite{dambrosio}{8}
\bibcite{nn_mode}{9}
\bibcite{pinn_paper}{10}
\bibcite{piee_paper}{11}
\bibcite{pimm_paper}{12}
\@writefile{lof}{\contentsline {figure}{\numberline {5}{\ignorespaces \it  Current status of $K_L\to \pi ^0l\mathaccent "7016\relax l$ searches.  }}{8}}
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