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Revision 322011-01-26 - PatrickJussel

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S.Haywood at rl.ac.uk (or failing that, edward.moyse at cern.ch)
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Discovery potential of h/H/A->ττ->ll 4ν

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Revision 312010-12-20 - PeterJones

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Revision 302009-12-01 - CalebLeeParnellLampenExCern

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Discovery potential of h/H/A->ττ->ll 4ν

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Revision 292009-05-19 - WolfgangMader

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Figure 5: Comparison of the pTmiss, x1 x1 , and mττ spectra for events of type Z->μμ and Z->ττ.Good agreement within the statistical uncertainties is observed.

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Figure 6: Comparison of the mττ shape for Z->ττ->μμ + X , Z->ττ-> ee + X , and Z->ττ->μe+X events. Good agreement is observed within the statistical uncertainties of the samples used.
 

Systematic Uncertainties

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Revision 282009-05-19 - WolfgangMader

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Analysis of the Exclusive Lepton Lepton Final State

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Introduction

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Figure 1: Systematic uncertainty on the signal cross-section for associated Higgs boson production as a function of mA . The dashed line corresponds to the contribution from the scale uncertainty, the dash-dotted line to that introduced by the uncertainty on the parton distribution functions, and the solid line is the sum of both contributions added in quadrature.
 

Preselection

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Event Selection

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Figure 2: Invariant mτ+ τ- distribution for a Higgs boson of mass mA = 130 GeV (left) after preselection cuts. The width has been determined by a fit of a single Gaussian to the peak region of the distribution. The right-hand plot shows the mτ+ τ- distribution as a function of the pT of the Higgs boson.
 
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Estimation of Z->ττ Background from Data

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Figure 4: Distribution of the invariant dilepton mass mll (left). The shaded area illustrates the distribution from Z->μμ events, and the solid line that from signal events. The contribution from Z->τ+τ- and tt events is illustrated by the dashed and dotted lines, respectively. The cut on the invariant ll mass is indicated by the solid vertical lines. The distribution of pTmiss in the calorimeter for Z->μμ and Z->ττ->μμ + X events (right). All plots shown are after preselection cuts.
 

Systematic Uncertainties

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Revision 272009-04-15 - WolfgangMader

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Revision 262009-02-05 - WolfgangMader

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Revision 252009-02-05 - WolfgangMader

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Discovery potential of h/H/A->ττ->ll 4ν (HG7)

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Discovery potential of h/H/A->ττ->ll 4ν

 
This page contains approved plots and results in the order as they appear in the CSC note. Only the CSC note contains all the relevant information and should thus be consulted if one of the plots is used.

Revision 242009-02-02 - WolfgangMader

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Revision 232009-01-30 - WolfgangMader

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Discovery potential of h/H/A->ττ->ll 4ν (HG7)

 
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Revision 222009-01-29 - WolfgangMader

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Table 2: Cross-section in fb passing the preselection criteria. The numbers for the signal samples are given assuming tanβ=20. In the event samples marked '2μ filter' two muons are required to be present at generator level. The numbers marked with (*) were obtained using cut factorization.
 
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Cross-section in fb passing the preselection criteria. The numbers for the signal samples are given assuming tanβ=20. In the event samples marked '2μ filter' two muons are required to be present at generator level. The numbers marked with (*) were obtained using cut factorization.
 

Event Selection

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Table 3: Accepted cross-section in fb for optimized cuts for mA=130GeV and tanβ=20. The values of the cuts applied are stated for the ee/μμ (upper row) and eμ (lower row) subchannels. In case only one number is given it applies to all leptonic subchannels.
 
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Accepted cross-section in fb for optimized cuts for mA=130GeV and tanβ=20. The values of the cuts applied are stated for the ee/μμ (upper row) and eμ (lower row) subchannels. In case only one number is given it applies to all leptonic subchannels.
 

Selection Results

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Table 4: Accepted cross-section for all Higgs boson mass hypotheses analyzed. The cross-section in fb for signal and background after all selection cuts is given (except for the cut on the mass window) for tanβ=20.
 
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Accepted cross-section for all Higgs boson mass hypotheses analyzed. The cross-section in fb for signal and background after all selection cuts is given (except for the cut on the mass window) for tanβ=20.
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Figure 3: Invariant mτ τ distribution for Higgs boson candidates with nominal masses as indicated in the plots. The distributions are shown after all selection cuts for tanβ=20. The vertical lines indicate the mass window used for calculating the signal significance.
 
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Invariant mτ τ distribution for Higgs boson candidates with nominal masses as indicated in the plots. The distributions are shown after all selection cuts for tanβ=20. The vertical lines indicate the mass window used for calculating the signal significance.
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Systematic Uncertainties

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Table 5: Effects of systematic uncertainties for different Higgs boson masses for tanβ=20. The effects of the systematic uncertainties considered are listed in percent. The total uncertainty is obtained by adding the individual contributions in quadrature.
 
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Estimation of the Z-> ττ Background from Data

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Results and Discovery Potential

 
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Invariant mτ τ distribution for Higgs boson
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Figure 7: The five σ discovery potential (left) and the 95% exclusion limit (right) as a function of mA and tanβ. The solid line represents the main result of the analysis. The dashed lines indicate the discovery potential and exclusion limit including an addition 10% uncertainty on the tt cross-section. The bands represent the influence of the systematic uncertainty on the signal cross-section.
 
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Results and Discovery Potential

 
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The discovery potential as a function of mA. The solid
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Figure 9: The discovery potential as a function of mA. The solid
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The five σ discovery potential (left) and the 95% exclusion limit (right) as a function of mA and tanβ. The solid line represents the main result of the analysis. The dashed lines indicate the discovery potential and exclusion limit including an addition 10% uncertainty on the tt cross-section. The bands represent the influence of the systematic uncertainty on the signal cross-section.

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Results and Discovery Potential

Differential cross-section distributions of $m_\mathrm{vis}$ for Higgs boson mass hypotheses of $m_A=130\GeV$ (top), $m_A=150\GeV$ (middle), and $m_A=200\GeV$(bottom) for $\tan\beta$ as indicated in the plots. For light Higgs boson masses the contribution from direct production processes dominates over that from $b$ quark associated production, while for $m_A=200\GeV$ the situation is reversed.

 
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The five $\sigma$ discovery potential (left) and the $95\%$ exclusion limit (right) as a function of $m_A$ and $\tan\beta$. The solid line represents the main result of the analysis. The dashed lines indicate the discovery potential and exclusion limit including an addition $10\%$ uncertainty on the $t\bar t$ cross-section. The bands represent the influence of the systematic uncertainty on the signal cross-section.
 
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Revision 212009-01-29 - WolfgangMader

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Cross-section in $\mathrm{fb}$ passing the preselection criteria. The numbers for the signal samples are given assuming $\tan\beta=20$. In the event samples marked \lq 2$\mu$ filter\rq, two muons are required to be present at generator level. The numbers marked with (*) were obtained using cut factorization.
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Cross-section in fb passing the preselection criteria. The numbers for the signal samples are given assuming tanβ=20. In the event samples marked '2μ filter' two muons are required to be present at generator level. The numbers marked with (*) were obtained using cut factorization.
 

Event Selection

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Accepted cross-section in $\mathrm{fb}$ for optimized cuts for $m_{A}=130$ GeV and $\tan\beta=20$. The values of the cuts applied are stated for the $ee/\mu\mu$ (upper row) and $e\mu$ (lower row) subchannels. In case only one number is given it applies to all leptonic subchannels.
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Accepted cross-section in fb for optimized cuts for mA=130GeV and tanβ=20. The values of the cuts applied are stated for the ee/μμ (upper row) and eμ (lower row) subchannels. In case only one number is given it applies to all leptonic subchannels.
 

Selection Results

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Accepted cross-section for all Higgs boson mass hypotheses analyzed. The cross-section in fb for signal and background after all selection cuts is given (except for the cut on the mass window) for tanβ=20.
 
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Invariant $m_{\tau^+\tau^-}$ distribution for Higgs boson candidates with nominal masses as indicated in the plots. The distributions are shown after all selection cuts for $\tan\beta=20$. The vertical lines indicate the mass window used for calculating the signal significance.
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Invariant mτ τ distribution for Higgs boson candidates with nominal masses as indicated in the plots. The distributions are shown after all selection cuts for tanβ=20. The vertical lines indicate the mass window used for calculating the signal significance.
 

Systematic Uncertainties

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Effects of systematic uncertainties for different Higgs boson masses for tanβ=20. The effects of the systematic uncertainties considered are listed in percent. The total uncertainty is obtained by adding the individual contributions in quadrature.
 
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Invariant $m_{\tau^+\tau^-}$ distribution for Higgs boson masses of $110\GeV$ (left) and $130\GeV$ (right) after subtraction of the $Z\to\tau^+\tau^-$ background as described in the text. The dots
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Invariant mτ τ distribution for Higgs boson masses of 110GeV (left) and 130GeV (right) after subtraction of the Z->ττ background as described in the text. The dots
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The five $\sigma$ discovery potential (left) and the $95\%$ exclusion limit (right) as a function of $m_A$ and $\tan\beta$. The
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  Cutflow for the background (top) and signal (bottom) samples. The numbers given correspond the cross-section in
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Systematic Uncertainties

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  Systematic uncertainty for the signal and background samples. For the default selection the result is given
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Results and Discovery Potential

Revision 202009-01-28 - WolfgangMader

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Revision 192009-01-27 - WolfgangMader

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Revision 172009-01-12 - WolfgangMader

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Revision 162008-12-17 - WolfgangMader

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Revision 152008-10-17 - WolfgangMader

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Cross-section in $\mathrm{fb}$ passing the preselection criteria as described in the text. All numbers are given for $\tan\beta=20$.
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Cross-section in $\mathrm{fb}$ passing the preselection criteria. The numbers for the signal samples are given assuming $\tan\beta=20$. In the event samples marked \lq 2$\mu$ filter\rq, two muons are required to be present at generator level. The numbers marked with (*) were obtained using cut factorization.
 

Event Selection

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Cutflow for optimized cuts for $m_{A}=130$ GeV and $\tan\beta=20$. The values of the cuts applied are stated for the $ee/\mu\mu$ and $e\mu$ subchannels. Where only one number is given it applies to all leptonic sub channels. The cross-sections given in $\mathrm{fb}$ correspond to the sum over all subchannels
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Accepted cross-section in $\mathrm{fb}$ for optimized cuts for $m_{A}=130$ GeV and $\tan\beta=20$. The values of the cuts applied are stated for the $ee/\mu\mu$ (upper row) and $e\mu$ (lower row) subchannels. In case only one number is given it applies to all leptonic subchannels.
 

Selection Results

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Summary of the selection results for all Higgs boson mass
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Accepted cross-section for all Higgs boson mass
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Effects of systematic uncertainties as described in the text for Higgs boson masses as given in the table for an integrated luminosity of $30\ifb$ and $\tan\beta=20$. In the first line the cross section in $\mathrm{fb}$ for selected signal and background events inside the mass window is given. The effects of the systematic uncertainties on that result are listed below in percent.
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Effects of systematic uncertainties for different Higgs boson masses for $\tan\beta=20$. The effects of the systematic uncertainties considered are listed in percent. The total uncertainty is obtained by adding the individual contributions in quadrature.
 
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Estimation of the Z-> ττ Background from Data

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The discovery potential as a function of $\tan\beta$ and for Higgs boson masses as indicated in the plots. The solid lines indicate the discovery potential including experimental systematic uncertainties. The dashed lines indicate the discovery potential including an additional systematic uncertainty on the $t\bar t$ cross-section. The bands indicate the impact of the systematic uncertainty on the signal cross-section.
 
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Discovery potential for Higgs bosons of mass $m_A=110\GeV$, $m_A=130\GeV$, $m_A=160\GeV$, and $m_A=200\GeV$ as a function of $\tan\beta$ in the $m_h^\mathrm{max}$ scenario, for an integrated luminosity of $30\ifb$, and for $\tan\beta=20$. The bands indicate the impact from the uncertainty on the signal and background cross-sections.
 
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The significance for a Higgs boson discovery as a function of $m_A$ for $\tan\beta$ values of $20$, $35$, and $45$ in the $m_h^\mathrm{max}$ scenario and for an integrated luminosity of $30\ifb$.
>
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The discovery potential as a function of $m_A$. The solid lines indicate the discovery potential including experimental systematic uncertainties for $\tan\beta$ values as indicated in the plots. The dashed lines indicate the discovery potential including an additional systematic uncertainty on the $t\bar t$ cross-section of $10\%$. The bands indicate the impact of the systematic uncertainty on the signal cross-section.
 
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The 95\% exclusion limit (dashed line) and the five sigma discovery potential (solid line) for Higgs bosons as a function of $m_A$ without (left) and with (right) systematic uncertainties taken into account and for an integrated luminosity of $30\ifb$. The exclusion limit set by the LEP experiments is indicated by the dotted line.
>
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The five $\sigma$ discovery potential (left) and the $95\%$ exclusion limit (right) as a function of $m_A$ and $\tan\beta$. The solid line represents the main result of the analysis. The dashed lines indicate the discovery potential and exclusion limit including an addition $10\%$ uncertainty on the $t\bar t$ cross-section. The bands represent the influence of the systematic uncertainty on the signal cross-section.
 
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Analysis of the Inclusive Lepton Lepton Final State

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Discovery Potential as a function of $\tan\beta$ (left) and in the luminosity vs. $\tan\beta$ plane (right) for Higgs boson mass hypotheses of $m_A=130\GeV$ (top), $m_A=150\GeV$ (middle), and $m_A=200\GeV$ (bottom). The significances were calculated using the Profile Likelihood method.
>
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The five $\sigma$ discovery potential (left) and the $95\%$ exclusion limit (right) as a function of $m_A$ and $\tan\beta$. The solid line represents the main result of the analysis. The dashed lines indicate the discovery potential and exclusion limit including an addition $10\%$ uncertainty on the $t\bar t$ cross-section. The bands represent the influence of the systematic uncertainty on the signal cross-section.
 
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Revision 142008-10-15 - WolfgangMader

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Analysis of the Exclusive Lepton Lepton Final State

Revision 132008-09-19 - WolfgangMader

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  the systematic uncertainties on that result are listed below in percent.
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Estimation of the Z-> ττ Background from Data

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Results and Discovery Potential

Revision 122008-09-16 - WolfgangMader

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PublicPlotsHG7

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Results and Discovery Potential

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 Discovery potential for Higgs bosons of mass $m_A=110\GeV$, $m_A=130\GeV$, $m_A=160\GeV$, and $m_A=200\GeV$ as a function of $\tan\beta$ in the $m_h^\mathrm{max}$ scenario, for an
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Analysis of the Inclusive Lepton Lepton Final State

Selection Results

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Revision 112008-08-26 - WolfgangMader

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Revision 102008-08-25 - WolfgangMader

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Revision 92008-08-23 - WolfgangMader

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Revision 82008-07-23 - WolfgangMader

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Revision 72008-04-28 - WolfgangMader

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Revision 62008-04-28 - WolfgangMader

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I
 Invariant $m_{\tau^+\tau^-}$ distribution for Higgs boson candidates with nominal masses as indicated in the plots. The distributions are shown after all selection cuts for
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Revision 52008-04-27 - WolfgangMader

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Systematic uncertainties on the normalization of the $Z\to\tau^+\tau^-$ background for Higgs boson masses of $m_A=110\GeV$ and $m_A=130\GeV$. The cross section in $\mathrm{fb}$ for an integrated luminosity of $30\ifb$ is given in the first line. The effect of the systematic uncertainties on that result is given in
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Effects of systematic uncertainties as described in the text for Higgs boson masses as given in the table for an integrated luminosity of $30\ifb$ and $\tan\beta=20$. In the first line the cross section in $\mathrm{fb}$ for selected signal and background events inside the mass window is given. The effects of the systematic uncertainties on that result are listed below in
  percent.

Estimation of the Z-> ττ Background from Data

Revision 42008-04-27 - WolfgangMader

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Analysis of the Exclusive Lepton Lepton Final State

Preselection

Revision 32008-04-27 - WolfgangMader

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Analysis of the Exclusive Lepton Lepton Final State

Preselection

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Selection Results

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  Summary of the selection results for all Higgs boson mass hypotheses analyzed. The cross-section in $\mathrm{fb}$ for signal
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  Systematic uncertainties on the normalization of the $Z\to\tau^+\tau^-$ background for Higgs boson masses of $m_A=110\GeV$
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  Invariant $m_{\tau^+\tau^-}$ distribution for Higgs boson masses of $110\GeV$ (left) and $130\GeV$ (right) after subtraction
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Results and Discovery Potential

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  Discovery potential for Higgs bosons of mass $m_A=110\GeV$, $m_A=130\GeV$, $m_A=160\GeV$, and $m_A=200\GeV$ as a
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  The 95\% exclusion limit (dashed line) and the five sigma discovery potential (solid line) for Higgs bosons as a function of
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Analysis of the Inclusive Lepton Lepton Final State

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  Differential cross-section distributions of $m_\mathrm{vis}$ for Higgs boson mass
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  Discovery Potential as a function of $\tan\beta$ (left) and in the luminosity vs. $\tan\beta$ plane (right) for Higgs boson mass

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Analysis of the Exclusive Lepton Lepton Final State

Preselection

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Cross-section in $\mathrm{fb}$ passing the preselection criteria as described in the text. All numbers are given for $\tan\beta=20$.
 

Event Selection

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Cutflow for optimized cuts for $m_{A}=130$ GeV and $\tan\beta=20$. The values of the cuts applied are stated for the $ee/\mu\mu$ and $e\mu$ subchannels. Where only one number is given it applies to all leptonic sub channels. The cross-sections given in $\mathrm{fb}$ correspond to the sum over all subchannels
 

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Text Summary of the selection results for all Higgs boson mass hypotheses analyzed. The cross-section in $\mathrm{fb}$ for signal and background after all selection cuts is given (except for the cut on the mass window) for $\tan\beta=20$. In the cases where zero events were left, the $95\%$ Poisson upper limit is given as statistical uncertainty.
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Invariant $m_{\tau^+\tau^-}$ distribution for Higgs boson candidates with nominal masses as indicated in the plots. The distributions are shown after all selection cuts for $\tan\beta=20$. The vertical lines indicate the mass window used for calculating the signal significance.
 

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Systematic uncertainties on the normalization of the $Z\to\tau^+\tau^-$ background for Higgs boson masses of $m_A=110\GeV$ and $m_A=130\GeV$. The cross section in $\mathrm{fb}$ for an integrated luminosity of $30\ifb$ is given in the first line. The effect of the systematic uncertainties on that result is given in percent.
 

Estimation of the Z-> ττ Background from Data

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Invariant $m_{\tau^+\tau^-}$ distribution for Higgs boson masses of $110\GeV$ (left) and $130\GeV$ (right) after subtraction of the $Z\to\tau^+\tau^-$ background as described in the text. The dots with error bars is the residual spectrum after background subtraction, the dark shaded area the signal as predicted from Monte Carlo, and the light shaded area is the remaining background from $t\bar t$ processes. In both plots $\tan\beta=20$ has been assumed.
 

Results and Discovery Potential

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Discovery potential for Higgs bosons of mass $m_A=110\GeV$, $m_A=130\GeV$, $m_A=160\GeV$, and $m_A=200\GeV$ as a function of $\tan\beta$ in the $m_h^\mathrm{max}$ scenario, for an integrated luminosity of $30\ifb$, and for $\tan\beta=20$. The bands indicate the impact from the uncertainty on the signal and background cross-sections.
 
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The significance for a Higgs boson discovery as a function of $m_A$ for $\tan\beta$ values of $20$, $35$, and $45$ in the $m_h^\mathrm{max}$ scenario and for an integrated luminosity of $30\ifb$.
 
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The 95\% exclusion limit (dashed line) and the five sigma discovery potential (solid line) for Higgs bosons as a function of $m_A$ without (left) and with (right) systematic uncertainties taken into account and for an integrated luminosity of $30\ifb$. The exclusion limit set by the LEP experiments is indicated by the dotted line.
 

Analysis of the Inclusive Lepton Lepton Final State

Selection Results

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Cutflow for the background (top) and signal (bottom) samples. The numbers given correspond the cross-section in $\mathrm{fb}$ after each cut. For the signal samples $\tan\beta=45$ is assumed.
 

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Systematic uncertainty for the signal and background samples. For the default selection the result is given as cross-section in $\mathrm{fb}$ for $\tan\beta=45$. For each systematic uncertainty the variation is given in percent with respect to the nominal value.
 

Results and Discovery Potential

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Differential cross-section distributions of $m_\mathrm{vis}$ for Higgs boson mass hypotheses of $m_A=130\GeV$ (top), $m_A=150\GeV$ (middle), and $m_A=200\GeV$(bottom) for $\tan\beta$ as indicated in the plots. For light Higgs boson masses the contribution from direct production processes dominates over that from $b$ quark associated production, while for $m_A=200\GeV$ the situation is reversed.
 
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Discovery Potential as a function of $\tan\beta$ (left) and in the luminosity vs. $\tan\beta$ plane (right) for Higgs boson mass hypotheses of $m_A=130\GeV$ (top), $m_A=150\GeV$ (middle), and $m_A=200\GeV$ (bottom). The significances were calculated using the Profile Likelihood method.
 
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Revision 12008-04-25 - WolfgangMader

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Analysis of the Exclusive Lepton Lepton Final State

Preselection

Event Selection

Selection Results

Text Text
Text Text

Systematic Uncertainties

Estimation of the Z-> ττ Background from Data

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Results and Discovery Potential

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Analysis of the Inclusive Lepton Lepton Final State

Selection Results

Systematic Uncertainties

Results and Discovery Potential

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Major updates:
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