Difference: PublicHGPlotsAtlPhysPub2010006 (1 vs. 5)

Revision 52011-01-26 - PatrickJussel

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Expected Sensitivity in Light Charged Higgs Boson Searches for H+→τ+ν and H+→cs with Early LHC Data at the ATLAS Experiment

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Revision 42010-12-20 - PeterJones

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Revision 32010-06-22 - CalebLeeParnellLampenExCern

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  This page contains approved plots and results as they appear in the ATL-PHYS-PUB-2010-006 note. Only the note contains all the relevant information and should thus be consulted if one of the plots is used. Click on an image to download in eps format. Please contact the HSG Documentation manager if you find any errors on this page.
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Figure 1 contains D0 and CDF results. If required, please retrieve up to date results from their respective publications.
 
Figure 1: The 95% confidence level upper limits on the branching ratio ${\cal B}(t \rightarrow bH^{+})$ versus $m_{H^{+}}$, assuming ${\cal B}(H^+ \rightarrow c\bar{s})=1$ (left, CDF) and ${\cal B}(H^+ \rightarrow \tau^+ \nu)=1$ (right, D0) for the charged Higgs boson. The CDF study [7] used a $2.2fb^{-1}$ dataset while the D0 study [8] used a $1 fb^{-1}$ dataset.

Revision 22010-06-21 - CalebLeeParnellLampenExCern

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Prospects for Higgs Boson Searches using the H->WW*->lνlν Decay Mode with the ATLAS Detector for 10TeV

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Expected Sensitivity in Light Charged Higgs Boson Searches for H+→τ+ν and H+→cs with Early LHC Data at the ATLAS Experiment

 
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This page contains approved plots and results as they appear in the ATL-PHYS-PUB-2010-005 note. Only the note contains all the relevant information and should thus be consulted if one of the plots is used. Click on an image to download in eps format.

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This page contains approved plots and results as they appear in the ATL-PHYS-PUB-2010-006 note. Only the note contains all the relevant information and should thus be consulted if one of the plots is used. Click on an image to download in eps format. Please contact the HSG Documentation manager if you find any errors on this page.
 

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Figure 1: The 95% confidence level upper limits on the branching ratio ${\cal B}(t \rightarrow bH^{+})$ versus $m_{H^{+}}$, assuming ${\cal B}(H^+ \rightarrow c\bar{s})=1$ (left, CDF) and ${\cal B}(H^+ \rightarrow \tau^+ \nu)=1$ (right, D0) for the charged Higgs boson. The CDF study [7] used a $2.2fb^{-1}$ dataset while the D0 study [8] used a $1 fb^{-1}$ dataset.
 

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Figure 2: At left, the dijet mass templates (normalized to a unit area) for the reconstructed $H^{+}$ and $W$ bosons. At right, the dijet mass templates (normalized to a unit area) for $H^{+}$ and $W$ after fitting. In the fitted distributions, a cut was made on the $\chi^{2}$ of the dijet mass fitter at 10 and we require the reconstructed top top mass on the hadronic side to the smaller than 195GeV.
 

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Figure 3: Example likelihood shape normalized to have maximum at 1 (solid line) and likelihood integral (dotted line) as a function of positive ${\cal B}(t \rightarrow bH^{+})$ for one PE. In both cases the maximum value is normalised to one. The arrow shows the position of the 95% CL upper limit from this particular PE.
 
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Figure 4: At left, an example likelihood shape for one PE before (solid line) and after (dotted line) systematic smearing. The solid and dotted arrows show the respective 95% CL upper limit on ${\cal B}(t \rightarrow bH^{+})$ for each PE assuming a $H^+$ mass of 130GeV. The mean (solid line) is taken as the expected value given a null-Higgs hypotheis. The dotted and dashed lines show the values of ${\cal B}(t \rightarrow bH^{+})$ which contain 68% and 95% of entries respectively.
 
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Figure 5: Left, di-jet mass as a function of the number of additional vertices in the event. The linear fit was used to derive a correction to the jet energies. Right, $W$ mass template from SM $t\bar{t}$ background events after correction of the jet energies.
 
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Figure 6: At left, the normalized $cos\theta{}^{*}_{l}$ distribution of final state electrons and muons in dilepton $t\bar{t}$ events, coming from $W\rightarrow{}l\nu{}_{l}$ (dotted line), $W \rightarrow \tau^{+}\nu \rightarrow l^{+}\nu\bar{\nu}\nu$ (dashed line) and $H^{+} \rightarrow \tau^+\nu \rightarrow l^{+}\nu\bar{\nu}\nu$ (full line). Note that only the normalized $cos \theta^{*}_{l}$ distribution associated to $W\rightarrow l\nu_l$ follows Equation (4). At right, generator-level $cos\theta^{*}_{l}$ distribution of the final state electrons and muons in dilepton $t\bar{t}$ events, assuming a correct assignment of the various decay products, in the SM (dashed line) and with a 130GeV charged Higgs boson in the top quark decays with ${\cal B}(t \rightarrow bH^{+})$ = 17% (full line).
 

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Figure 7: At left, the normalized $m^{H^{+}}_{T2}$ distributions for $t\bar{t}\rightarrow bW^+ \bar{b}W^- \rightarrow bl^+ \nu_l + bl^-\bar{\nu}_l$ (dotted line) and $t\bar{t}\rightarrow bW^{+}\bar{b}H^-\rightarrow bl^+\nu_l + \bar{b}\tau^- \bar{\nu}_\tau$ (full line). At right, generator-level distributions of the generalized transverse mass, assuming a correct assignment of the various decay products, in the SM (dashed line) and with a 130GeV charged Higgs boson in the top quark decays, with ${\cal B}(t \rightarrow bH^{+})$ = 17% (full line).
 

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Figure 8: Comparison of the $cos\theta{}^{*}_{l}$ and generalized transverse mass distributions, as obtained from the scaled MC samples and the TopMixing sample in the $Z$ sideband (the $Wbb$ and $Zbb$ backgrounds are shown by the darker shaded histograms). Dilepton $t\bar{t} \rightarrow H^+ W$ events were later added to the TopMixing sample, however this sideband is not sensitive to the signal.
 

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Figure 9: Comparison of the $cos\theta{}^{*}_{l}$ and generalized transverse mass distributions, as obtained from the scaled MC samples (with no $t\bar{t} \rightarrow H^+ W$ event) and the TopMixing sample in the $t\bar{t}$ sideband, however with no cut on $cos\theta{}^{*}_{l}$.
 

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Figure 10: Comparison of the $cos\theta{}^{*}_{l}$ distribution in the SM case (dashed line) and as obtained when assuming $m_{H^+}$ = 130GeV together with ${\cal B}(t \rightarrow bH^{+})$ = 17% (filled histogram). All selection cuts are applied, except the one on $cos\theta{}^{*}_{l}$.
 
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d 95% CL upper limits for ${\cal B}(t \rightarrow b H^{+})$
 
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Figure 11: Comparison of the generalized transverse mass distributions in the SM case (dashed line) and as obtained when assuming $m_{H^+}$ = 130GeV together with ${\cal B}(t \rightarrow b H^{+})$ = 17% (filled histogram). All selection cuts are applied, except the one on $cos\theta{}^{*}_{l}$.
 

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Figure 12: Determination of the branching ratio upper limit with (dashed line) and without (solid line) systematic uncertainties, for a 130GeV charged Higgs boson.
 
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Figure 13: Expected 95% CL upper limits for ${\cal B}(t \rightarrow b H^{+})$ as a function of $m_{H^+}$ in ATLAS, using the early LHC data (i.e. $\int dt \mathcal{L}=200$~pb$^{-1}$ and $\sqrt{s}$ = 10TeV), in the $H^+ \rightarrow c\bar{s}$ (left) and $H^+ \rightarrow \tau^+ \nu \rightarrow l + \nu s$ (right) channels. Also shown for reference are the current Tevatron upper limits on ${\cal B}(t \rightarrow b H^{+})$. No pile-up is included here.
 
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META TOPICPARENT name="HiggsMaterialForPublicTalks"
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Prospects for Higgs Boson Searches using the H->WW*->lνlν Decay Mode with the ATLAS Detector for 10TeV

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This page contains approved plots and results as they appear in the ATL-PHYS-PUB-2010-005 note. Only the note contains all the relevant information and should thus be consulted if one of the plots is used. Click on an image to download in eps format.

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<!--For significant updates to the topic, consider adding your 'signature' (beneath this editing box)-->
Major updates:
-- CalebLampen - 21-Jun-2010

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