(r2) PublicHGPlotsAtlPhysPub2010011 < AtlasPublic

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---+!!<nop>Discovery Potential of A/H&rarr;&tau;<sup>+</sup>&tau;<sup>-</sup>&rarr;lh in ATLAS

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  <div style="width:600px; background: rgb(220,230,220); border: 5px solid silver; float: center;">
    *This page contains approved plots and results as they appear in the [[http://cdsweb.cern.ch/record/1279115][ATL-PHYS-PUB-2010-011]] 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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<div align="center" style="width:800px">
<a href="%ATTACHURL%/objects_trigger.eps">
	<img src="%ATTACHURL%/objects_trigger.png" width=60%></img></a>
<div style="width:80%;">
*Figure 1:* Trigger efficiency as a function of %$p_T$% for electrons (left) and muons (right). For the extraction of the trigger of the trigger efficiency, a Gaussian error function is fit to the data.  In the plateau region, a trigger efficiency of ~ 98% (~ 81%) for electrons (muons) is obtained.
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<div align="center" style="width:800px">
<a href="%ATTACHURL%/selection_noBT_dPhi.eps">
	<img src="%ATTACHURL%/selection_noBT_dPhi.png" width=33%></img></a>
<a href="%ATTACHURL%/selection_noBT_MET.eps">
	<img src="%ATTACHURL%/selection_noBT_MET.png" width=33%></img></a>
<a href="%ATTACHURL%/selection_noBT_tauPt.eps">
	<img src="%ATTACHURL%/selection_noBT_tauPt.png" width=33%></img></a>
<a href="%ATTACHURL%/selection_BT_dPhi.eps">
	<img src="%ATTACHURL%/selection_BT_dPhi.png" width=33%></img></a>
<a href="%ATTACHURL%/selection_BT_MET.eps">
	<img src="%ATTACHURL%/selection_BT_MET.png" width=33%></img></a>
<a href="%ATTACHURL%/selection_BT_tauPt.eps">
	<img src="%ATTACHURL%/selection_BT_tauPt.png" width=33%></img></a>
<div style="width:80%;">
*Figure 2:* Optimized selection criteria for %$\Delta\Phi_{\ell,\tau}$% (left), %$E_{T}^{\tau}$% (right) for a Higgs boson mass hypothesis of %$m_A$% = 300 !GeV in the non-b-tagged (top row) and b-tagged (bottom row) analysis. The chosen selection cuts are shown as horizontal black lines.
</div>
</div>

<div align="center" style="width:800px">
<a href="%ATTACHURL%/background_TransMassWControl.eps">
	<img src="%ATTACHURL%/background_TransMassWControl.png" width=49%></img></a>
<a href="%ATTACHURL%/background_WControlMassDist.eps">
	<img src="%ATTACHURL%/background_WControlMassDist.png" width=49%></img></a>
<div style="width:80%;">
*Figure 3:* Transverse mass distribution in the W+jets control region before the transverse-mass window cut is applied (left) and the invariant %$m_{\tau\tau}$% distribution for W+jets events in the control and signal regions (right).
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</div>

<div align="center" style="width:800px">
<a href="%ATTACHURL%/background_refhist3.eps">
	<img src="%ATTACHURL%/background_refhist3.png" width=49%></img></a>
<a href="%ATTACHURL%/background_rescaling_e_mtt.eps">
	<img src="%ATTACHURL%/background_rescaling_e_mtt.png" width=49%></img></a>
<div style="width:80%;">
*Figure 4:* Left: %$Z \to \tau \tau$% reference histogram showing the visible energy of the hadronically decaying %$\tau$% lepton versus that of the light lepton in the %$Z$%-boson rest frame, for 0.2 < |%$cos \theta_{GJ}$%| < 0.4. Right: Invariant %$m_{\tau\tau}$% distribution for %$Z \to \tau \tau$% events (shaded rectangles) compared with %$Z\to e e$% events after rescaling (points with error bars).
</div>
</div>

<div align="center" style="width:800px">
<a href="%ATTACHURL%/background_control300.eps">
	<img src="%ATTACHURL%/background_control300.png" width=49%></img></a>
<a href="%ATTACHURL%/background_result300.eps">
	<img src="%ATTACHURL%/background_result300.png" width=49%></img></a>
<div style="width:80%;">
*Figure 5:* Jet multiplicity distribution in the control region (left) and in the signal region (right). In the control region a high purity of %$t\bar{t}$% events is observed. Good agreement between the predicted and the observed number of %$t\bar{t}$% events is achieved in the signal region, in particular for the one-jet and the two-jet bins relevant to this analysis.
</div>
</div>

<div align="center" style="width:800px">
<a href="%ATTACHURL%/results_Contour_FinalResult_ll_smooth.eps">
	<img src="%ATTACHURL%/results_Contour_FinalResult_ll_smooth.png" width=49%></img></a>
<div style="width:80%;">
*Figure 6:* The five-&sigma; discovery potential as a function of tan&beta; and %$m_A$%. The solid green line is the result of the lepton-hadron analysis. The dashed green lines indicates the effect of the theoretical uncertainty on the signal cross section. The red line gives the results for the fully correlated treatment of systematic
uncertainties. The dash-dotted black line shows the discovery potential without inclusion of systematic uncertainties for comparison with previous results. The results from the lepton-lepton analysis are superimposed as blue lines. The solid line indicates the result including only experimental systematic uncertainties and the dashed line indicates the result including a 10% theoretical uncertainty on the %$t\bar{t}$% cross-section.
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</div>

<div align="center" style="width:800px">
<a href="%ATTACHURL%/results_MI_mA150_BTag0.eps">
	<img src="%ATTACHURL%/results_MI_mA150_BTag0.png" width=49%></img></a>
<a href="%ATTACHURL%/results_MI_mA150_BTag1.eps">
	<img src="%ATTACHURL%/results_MI_mA150_BTag1.png" width=49%></img></a>
<div style="width:80%;">
*Figure 7:* Invariant mass of the %$\tau\tau$% system in the non-b-tagged (left) and the b-tagged analysis (right). The size of the signal contribution is scaled to a tan&beta; value of 14, corresponding to the value necessary for a five-&sigma; discovery. The mass window used to calculate the significance is indicated by vertical black lines. 
</div>
</div>

<div align="center" style="width:800px">
<a href="%ATTACHURL%/results_MI_mA200_BTag0.eps">
	<img src="%ATTACHURL%/results_MI_mA200_BTag0.png" width=49%></img></a>
<a href="%ATTACHURL%/results_MI_mA200_BTag1.eps">
	<img src="%ATTACHURL%/results_MI_mA200_BTag1.png" width=49%></img></a>
<div style="width:80%;">
*Figure 8:* Invariant mass of the %$\tau\tau$% system in the non-b-tagged (left) and the b-tagged analysis (right). The size of the signal contribution is scaled to a tan&beta; value of 14, corresponding to the value necessary for a five-&sigma; discovery. The mass window used to calculate the significance is indicated by vertical black lines. 
</div>
</div>

<div align="center" style="width:800px">
<a href="%ATTACHURL%/results_MI_mA300_BTag0.eps">
	<img src="%ATTACHURL%/results_MI_mA300_BTag0.png" width=49%></img></a>
<a href="%ATTACHURL%/results_MI_mA300_BTag1.eps">
	<img src="%ATTACHURL%/results_MI_mA300_BTag1.png" width=49%></img></a>
<div style="width:80%;">
*Figure 9:* Invariant mass of the %$\tau\tau$% system in the non-b-tagged (left) and the b-tagged analysis (right). The size of the signal contribution is scaled to a tan&beta; value of 14, corresponding to the value necessary for a five-&sigma; discovery. The mass window used to calculate the significance is indicated by vertical black lines. 
</div>
</div>

<div align="center" style="width:800px">
<a href="%ATTACHURL%/results_MI_mA450_BTag0.eps">
	<img src="%ATTACHURL%/results_MI_mA450_BTag0.png" width=49%></img></a>
<a href="%ATTACHURL%/results_MI_mA450_BTag1.eps">
	<img src="%ATTACHURL%/results_MI_mA450_BTag1.png" width=49%></img></a>
<div style="width:80%;">
*Figure 10:* Invariant mass of the %$\tau\tau$% system in the non-b-tagged (left) and the b-tagged analysis (right). The size of the signal contribution is scaled to a tan&beta; value of 14, corresponding to the value necessary for a five-&sigma; discovery. The mass window used to calculate the significance is indicated by vertical black lines. 
</div>
</div>

<div align="center" style="width:800px">
<a href="%ATTACHURL%/results_MI_mA600_BTag0.eps">
	<img src="%ATTACHURL%/results_MI_mA600_BTag0.png" width=49%></img></a>
<a href="%ATTACHURL%/results_MI_mA600_BTag1.eps">
	<img src="%ATTACHURL%/results_MI_mA600_BTag1.png" width=49%></img></a>
<div style="width:80%;">
*Figure 11:* Invariant mass of the %$\tau\tau$% system in the non-b-tagged (left) and the b-tagged analysis (right). The size of the signal contribution is scaled to a tan&beta; value of 14, corresponding to the value necessary for a five-&sigma; discovery. The mass window used to calculate the significance is indicated by vertical black lines. 
</div>
</div>

<div align="center" style="width:800px">
<a href="%ATTACHURL%/results_MI_mA800_BTag0.eps">
	<img src="%ATTACHURL%/results_MI_mA800_BTag0.png" width=49%></img></a>
<a href="%ATTACHURL%/results_MI_mA800_BTag1.eps">
	<img src="%ATTACHURL%/results_MI_mA800_BTag1.png" width=49%></img></a>
<div style="width:80%;">
*Figure 12:* Invariant mass of the %$\tau\tau$% system in the non-b-tagged (left) and the b-tagged analysis (right). The size of the signal contribution is scaled to a tan&beta; value of 14, corresponding to the value necessary for a five-&sigma; discovery. The mass window used to calculate the significance is indicated by vertical black lines. 
</div>
</div>

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*Major updates*:%BR%
-- Main.CalebLampen - 22-Jul-2010

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Attachments

Topic attachments
I	Attachment	History	Action	Size	Date	Who
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png	background_TransMassWControl.png	r1	manage	273.3 K	2010-07-22 - 17:14	CalebLeeParnellLampenExCern
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png	background_WControlMassDist.png	r1	manage	177.5 K	2010-07-22 - 17:15	CalebLeeParnellLampenExCern
eps	background_control300.eps	r1	manage	30.7 K	2010-07-22 - 18:02	CalebLeeParnellLampenExCern
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png	results_MI_mA600_BTag1.png	r1	manage	129.2 K	2010-07-22 - 17:40	CalebLeeParnellLampenExCern
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png	results_MI_mA800_BTag1.png	r1	manage	134.4 K	2010-07-22 - 17:39	CalebLeeParnellLampenExCern
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eps	selection_BT_dPhi.eps	r1	manage	23.0 K	2010-07-22 - 17:05	CalebLeeParnellLampenExCern
png	selection_BT_dPhi.png	r1	manage	191.5 K	2010-07-22 - 17:05	CalebLeeParnellLampenExCern
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eps	selection_noBT_MET.eps	r1	manage	21.2 K	2010-07-22 - 18:01	CalebLeeParnellLampenExCern
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eps	selection_noBT_dPhi.eps	r1	manage	21.4 K	2010-07-22 - 17:01	CalebLeeParnellLampenExCern
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png	selection_noBT_tauPt.png	r1	manage	187.8 K	2010-07-22 - 17:11	CalebLeeParnellLampenExCern

Topic revision: r2 - 2010-12-20 - PeterJones

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