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\relax
\global\@todotoctrue
\citation{Aad2015}
\citation{CMS-PAS-HIG-16-007}
\citation{ATLAS-CONF-2015-061}
\citation{HH_bbbb_ATLAS}
\citation{HH_bbgg_ATLAS}
\citation{chargedH_tb_ATLAS}
\citation{chargedH_tuanu_ATLAS}
\citation{HH_bbtautau_CMS}
\citation{HH_bbWW_CMS}
\citation{HH_bbbb_CMS}
\citation{Hmumu_ref_CMS}
\citation{Hbb_ref_CMS}
\citation{chargedH_tb_CMS}
\citation{diChargedH}
\citation{aa3photon}
\@writefile{toc}{\contentsline {section}{\numberline {1}Introduction}{1}}
\@writefile{lof}{\contentsline {figure}{\numberline {1}{\ignorespaces Run1 $m_A - tan\beta $ exclusion plane by (left) CMS experiment and (right) ATLAS experiment.}}{1}}
\newlabel{fig:MSSM_Run1}{{1}{1}}
\global\@todotoctrue
\@writefile{toc}{\contentsline {section}{\numberline {2}Search for neutral Higgs bosons $H/A \rightarrow \tau \tau $}{2}}
\@writefile{toc}{\contentsline {subsection}{\numberline {2.1}$\tau _{\rm had}$ reconstruction}{2}}
\@writefile{toc}{\contentsline {subsection}{\numberline {2.2}The $\tau _{\rm had}\tau _{\rm had}$, $\tau _{e}\tau _{\rm had}$, $\tau _{\mu }\tau _{\rm had}$ and $\tau _{e}\tau _{\mu }$ channels}{3}}
\@writefile{lof}{\contentsline {figure}{\numberline {2}{\ignorespaces (Left) Post--fit plot of the total transverse mass distribution in f the $\tau _{\rm had}\tau _{\rm had}$ channel by the ATLAS collaboration. (Right) Post--fit plot of the transverse mass distribution in the no b--tag category of the $\tau _{e}\tau _{\mu }$ channel by the CMS collaboration.}}{4}}
\newlabel{fig_1Htautau}{{2}{4}}
\@writefile{toc}{\contentsline {subsection}{\numberline {2.3}Results}{4}}
\@writefile{lof}{\contentsline {figure}{\numberline {3}{\ignorespaces Observed and expected 95\% CL upper limits on the product of cross section and the branching fraction $\sigma (pp\rightarrow \phi ) \times B(\phi \rightarrow \tau \tau )$ obtained by the ATLAS collaboriation (left) and by the CMS collaboriation (right) for the gluon-gluon fusion production.}}{4}}
\newlabel{fig_2aHtautau}{{3}{4}}
\global\@todotoctrue
\@writefile{lof}{\contentsline {figure}{\numberline {4}{\ignorespaces Observed and expected 95\% CL upper limits on the product of cross section and the branching fraction $\sigma (pp\rightarrow \phi ) \times B(\phi \rightarrow \tau \tau )$ obtained by the ATLAS collaboriation (left) and by the CMS collaboriation (right) for the b-associted production.}}{5}}
\newlabel{fig_2bHtautau}{{4}{5}}
\@writefile{lof}{\contentsline {figure}{\numberline {5}{\ignorespaces The expected and observed 95\% CL upper limits on tan$\beta $ as a function of $m_{A}$ in the MSSM $m_{h}^{mod+}$ scenario for ATLAS (left) and CMS (right).}}{5}}
\newlabel{fig_3Htautau}{{5}{5}}
\@writefile{toc}{\contentsline {section}{\numberline {3}Search for Higgs boson pair production}{5}}
\newlabel{ref:HHProduction}{{3}{5}}
\citation{HH_ATLAS_8TeV}
\citation{HH_CMS_8TeV}
\@writefile{lof}{\contentsline {figure}{\numberline {6}{\ignorespaces (left) ATLAS combination Higgs boson pair production in the $hh\ensuremath {\rightarrow }bb\ensuremath {\tau }\ensuremath {\tau }$, $\ensuremath {\gamma }\ensuremath {\gamma }W{W}^{*}$, $\ensuremath {\gamma }\ensuremath {\gamma }bb$, $bbbb$ channels with $8\,TeV$ data, (right) CMS Observed and expected 95\% CL upper limits on the product of cross section and the branching fraction $\sigma (gg\rightarrow X) \times B(X\rightarrow hh)$ obtained by different analyses assuming spin-0 hypothesis.}}{6}}
\newlabel{fig:HH_8TeV_Results}{{6}{6}}
\@writefile{toc}{\contentsline {subsection}{\numberline {3.1}$H\rightarrow hh \rightarrow bbbb$ channel}{6}}
\@writefile{toc}{\contentsline {subsection}{\numberline {3.2}$H\rightarrow hh \rightarrow bb\tau \tau $ channel}{6}}
\@writefile{lof}{\contentsline {figure}{\numberline {7}{\ignorespaces (left) CMS: The observed and expected upper limits on the cross section for a spin-2 resonance $H\rightarrow hh\rightarrow bbbb$ at a 95\% confidence level using data corresponding to an integrated luminosity of $2.3 fb^{?1}$ at $13 TeV$ using the asymptotic $CL_S$ method, (right) ATLAS: The expected and observed upper limit for $pp\rightarrow H\rightarrow hh\rightarrow bbbb$ with fixed $\Gamma _H = 1 GeV$, at the 95\% confidence level .}}{7}}
\newlabel{fig:HH_bbbb}{{7}{7}}
\@writefile{lof}{\contentsline {figure}{\numberline {8}{\ignorespaces Observed and expected 95\% CL upper limits on $\sigma (pp\rightarrow H) \times BR(H \rightarrow hh \rightarrow bb\tau \tau )$ from the combination of the three channels as a function of the mass of the resonance $m_H$}}{7}}
\newlabel{fig:HH_bbtt}{{8}{7}}
\@writefile{toc}{\contentsline {subsection}{\numberline {3.3}$H\rightarrow hh \rightarrow bbWW$ channel}{7}}
\@writefile{lof}{\contentsline {figure}{\numberline {9}{\ignorespaces Observed and expected 95\% CL upper limits on $\sigma (pp\rightarrow H) \times BR(H \rightarrow hh \rightarrow bbl\nu l\nu )$}}{8}}
\newlabel{fig:HH_bbWW}{{9}{8}}
\@writefile{toc}{\contentsline {subsection}{\numberline {3.4}$H\rightarrow hh \rightarrow bb\gamma \gamma $ channel}{8}}
\@writefile{lof}{\contentsline {figure}{\numberline {10}{\ignorespaces Observed and expected 95\% CL upper limits on $\sigma (pp\rightarrow H) \times BR(H \rightarrow hh \rightarrow bb\gamma \gamma )$}}{8}}
\newlabel{fig:HH_bbgg}{{10}{8}}
\global\@todotoctrue
\bibdata{mybib}
\bibcite{HH_CMS_8TeV}{1}
\bibcite{ATLAS-CONF-2015-061}{2}
\bibcite{diChargedH}{3}
\bibcite{HH_bbgg_ATLAS}{4}
\bibcite{HH_bbtautau_CMS}{5}
\bibcite{HH_bbWW_CMS}{6}
\bibcite{HH_bbbb_CMS}{7}
\bibcite{CMS-PAS-HIG-16-007}{8}
\bibcite{chargedH_tb_ATLAS}{9}
\bibcite{chargedH_tuanu_ATLAS}{10}
\bibcite{HH_bbbb_ATLAS}{11}
\bibcite{Aad2015}{12}
\bibcite{aa3photon}{13}
\bibcite{HH_ATLAS_8TeV}{14}
\bibcite{chargedH_tb_CMS}{15}
\bibcite{Hbb_ref_CMS}{16}
\bibcite{Hmumu_ref_CMS}{17}
\bibstyle{plain}
\@writefile{toc}{\contentsline {section}{\numberline {4}Conclusions}{9}}