PublicHGPlotsAtlPhysPub2009079 < AtlasPublic

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---+!!<nop>ATLAS searches for MSSM Higgs bosons decaying into SUSY cascades

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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/1165535][ATL-PHYS-PUB-2009-079]] 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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<div align="center" style="width:800px">
<a href="%ATTACHURL%/bratioAH.eps">
    <img src="%ATTACHURL%/bratioAH.png" width=50%></img></a>
<div style="width:80%;">
*Figure 1:* Example of %$A/H$% decay (%$A/H\rightarrow{}\tilde{\chi{}}^{0}_{2}\tilde{\chi{}}^{0}_{2}$%) with final state containing four leptons and undetectable particles.
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<div align="center" style="width:800px">
<a href="%ATTACHURL%/Xsec.vs.MA_tanb_8_10_20_30_x_Set1.eps">
    <img src="%ATTACHURL%/Xsec.vs.MA_tanb_8_10_20_30_x_Set1.png"width=45% ></img></a>
<a href="%ATTACHURL%/Br.vs.MA_tanb_8_10_20_30_x_Set1.eps">
    <img src="%ATTACHURL%/Br.vs.MA_tanb_8_10_20_30_x_Set1.png"  width=45%></img></a>
<div style="width:80%;">
*Figure 2:* Results at the generator level for <b>Set1</b>, as a function of %$m_A$% at tan&beta; = 8, 10, 20, 30. On the left, the Higgs boson %$A$% production cross section %$\sigma$%. On the right, the effective four lepton branching ratio, Br x &epsilon;.
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<div align="center" style="width:800px">
<a href="%ATTACHURL%/Xsec.x.Br.vs.MA_tanb_8_10_20_30_x_Set1.eps">
    <img src="%ATTACHURL%/Xsec.x.Br.vs.MA_tanb_8_10_20_30_x_Set1.png"width=45% ></img></a>
<a href="%ATTACHURL%/Xsec.x.Br.vs.MH_tanb_8_10_20_30_x_Set1.eps">
    <img src="%ATTACHURL%/Xsec.x.Br.vs.MH_tanb_8_10_20_30_x_Set1.png"width=45% ></img></a>
<a href="%ATTACHURL%/Xsec.x.Br.vs.SQG_LL_XX_tanb_20_Set1.eps">
    <img src="%ATTACHURL%/Xsec.x.Br.vs.SQG_LL_XX_tanb_20_Set1.png"width=45% ></img></a>
<a href="%ATTACHURL%/Xsec.x.Br.vs.MtH_tanb_8_10_20_30_x_Set1.eps">
    <img src="%ATTACHURL%/Xsec.x.Br.vs.MtH_tanb_8_10_20_30_x_Set1.png"width=45% ></img></a>
<div style="width:80%;">
*Figure 3:* Results at the generator level for <b>Set1</b>, as a function of %$m_{A}$%, at tan&beta; = 8, 10, 20, 30: the production cross section %$\sigma$% times the four lepton effective branching ratio Br x %$\epsilon$% for A events (top left); %$H$% events (top right); (%$\tilde{q}$%,%$\tilde{g}$%), (%$\tilde{\ell}$%,%$\tilde{\nu}$%),(%$\tilde{\chi}\tilde{\chi}$%,%$\tilde{q}$%/%$\tilde{g}\tilde{\chi}$%) events (bottom left); %$tH^{\pm}$% events (bottom right).
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<div align="center" style="width:800px">
<a href="%ATTACHURL%/Xsec.x.Br.vs.MA_tanb_5_15_25_35_45_Set2.eps">
    <img src="%ATTACHURL%/Xsec.x.Br.vs.MA_tanb_5_15_25_35_45_Set2.png"width=45% ></img></a>
<a href="%ATTACHURL%/Xsec.x.Br.vs.MtH_tanb_5_15_25_35_45_Set2.eps">
    <img src="%ATTACHURL%/Xsec.x.Br.vs.MtH_tanb_5_15_25_35_45_Set2.png"width=45% ></img></a>
<div style="width:80%;">
*Figure 4:* Results at the generator level for <b>Set2</b>, as a function of %$m_{A}$%, at tan&beta; = 5, 15, 25, 35, 45: the production cross section &sigma; times the four lepton effective branching ratio Br x &epsilon; for %$A$% events (left); %$tH^{\pm}$% events (right).
</div>
</div>


<div align="center" style="width:800px">
<a href="%ATTACHURL%/d0_muon_Cut_1_A_Set2.eps">
    <img src="%ATTACHURL%/d0_muon_Cut_1_A_Set2.png"width=45% ></img></a>
<a href="%ATTACHURL%/d0_muon_Cut_1_tt_Set2.eps">
    <img src="%ATTACHURL%/d0_muon_Cut_1_tt_Set2.png"width=45% ></img></a>
<a href="%ATTACHURL%/d0_elec_Cut_1_H_Set2.eps">
    <img src="%ATTACHURL%/d0_elec_Cut_1_H_Set2.png"width=45% ></img></a>
<a href="%ATTACHURL%/d0_elec_Cut_1_Zbb_Set2.eps">
    <img src="%ATTACHURL%/d0_elec_Cut_1_Zbb_Set2.png"width=45% ></img></a>
<div style="width:80%;">
*Figure 5:* <i>Point2 selection results.</i> Reconstructed transverse impact parameter significance, %$d0/\sigma_{d0}$%, distributions after cut 1, Section 7, for muons in %$A$% (top left) and %$t\bar{t}$% (top right) events; for electrons in %$H$% (bottom left) and %$Zb\bar{b}$% (bottom right) events. All distributions are normalized at %$\int\mathcal{L} = 300 fb^{-1}$%.
</div>
</div>


<div align="center" style="width:800px">
<a href="%ATTACHURL%/Minv_ll_Cut_2_A_Set2.eps">
    <img src="%ATTACHURL%/Minv_ll_Cut_2_A_Set2.png"width=45% ></img></a>
<a href="%ATTACHURL%/Minv_ll_Cut_2_ZZ_Set2.eps">
    <img src="%ATTACHURL%/Minv_ll_Cut_2_ZZ_Set2.png"width=45% ></img></a>
<a href="%ATTACHURL%/Minv_ll_Cut_2_H_Set2.eps">
    <img src="%ATTACHURL%/Minv_ll_Cut_2_H_Set2.png"width=45% ></img></a>
<a href="%ATTACHURL%/Minv_ll_Cut_2_Zbb_Set2.eps">
    <img src="%ATTACHURL%/Minv_ll_Cut_2_Zbb_Set2.png"width=45% ></img></a>
<div style="width:80%;">
*Figure 6:* <i>Point2 selection results.</i> Reconstructed dilepton invariant mass, %$M^{\ell\ell}_{inv}$%, distributions after cuts 1,2, Section 7, for %$A$% (top left), %$ZZ$% (top right), %$H$% (bottom left) and %$Zb\bar{b}$% (bottom right) events. All distributions are normalized at %$\int\mathcal{L} = 300 fb^{-1}$%. Bin width = 3 !GeV.
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<div align="center" style="width:800px">
<a href="%ATTACHURL%/ETmiss_Cut_3_A_Set2.eps">
    <img src="%ATTACHURL%/ETmiss_Cut_3_A_Set2.png"width=45% ></img></a>
<a href="%ATTACHURL%/ETmiss_Cut_3_ZZ_Set2.eps">
    <img src="%ATTACHURL%/ETmiss_Cut_3_ZZ_Set2.png"width=45% ></img></a>
<a href="%ATTACHURL%/ETmiss_Cut_3_Zbb_Set2.eps">
    <img src="%ATTACHURL%/ETmiss_Cut_3_Zbb_Set2.png"width=45% ></img></a>
<a href="%ATTACHURL%/ETmiss_Cut_3_SQG_Set2.eps">
    <img src="%ATTACHURL%/ETmiss_Cut_3_SQG_Set2.png"width=45% ></img></a>

<div style="width:80%;">
*Figure 7:* <i>Point2 selection results.</i> Reconstructed transverse missing energy, %$E^{miss}_{T}$%, after cuts 1,2,3, Section 7, for %$A$% (top left), %$ZZ$% (top right), %$Zb\bar{b}$% (bottom left), (%$\tilde{q},\tilde{g}$%) (bottom right) events. All distributions are normalized at %$\int\mathcal{L} = 300 fb^{-1}$%. Bin width = 1.5 !GeV.
</div>
</div>

<div align="center" style="width:800px">
<a href="%ATTACHURL%/Pt_muon_Cut_4_A_Set2.eps">
    <img src="%ATTACHURL%/Pt_muon_Cut_4_A_Set2.png"width=45% ></img></a>
<a href="%ATTACHURL%/Pt_muon_Cut_4_tt_Set2.eps">
    <img src="%ATTACHURL%/Pt_muon_Cut_4_tt_Set2.png"width=45% ></img></a>
<a href="%ATTACHURL%/Pt_elec_Cut_4_H_Set2.eps">
    <img src="%ATTACHURL%/Pt_elec_Cut_4_H_Set2.png"width=45% ></img></a>
<a href="%ATTACHURL%/Pt_elec_Cut_4_SQG_Set2.eps">
    <img src="%ATTACHURL%/Pt_elec_Cut_4_SQG_Set2.png"width=45% ></img></a>

<div style="width:80%;">
*Figure 8:* <i>Point2 selection results.</i> Reconstructed lepton transverse momentum (%$p_{T}^{\mu},p_{T}^{e}$%) distributions after cuts1,2,3,4, Section 7, for muons in %$A$% (top left) and %$t\bar{t}$% (top right) events; for electrons in %$H$% (bottom left) and (%$\tilde{q},\tilde{g}$%) events (bottom right) events. All distributions are normalized at %$\int\mathcal{L} = 300 fb^{-1}$%. Bin width = 1.5 !GeV.
</div>
</div>

<div align="center" style="width:800px">
<a href="%ATTACHURL%/Njet_Cut_5_A_Set2.eps">
    <img src="%ATTACHURL%/Njet_Cut_5_A_Set2.png"width=45% ></img></a>
<a href="%ATTACHURL%/Njet_Cut_5_SQG_Set2.eps">
    <img src="%ATTACHURL%/Njet_Cut_5_SQG_Set2.png"width=45% ></img></a>
<a href="%ATTACHURL%/Ptjet_Cut_5_H_Set2.eps">
    <img src="%ATTACHURL%/Ptjet_Cut_5_H_Set2.png"width=45% ></img></a>
<a href="%ATTACHURL%/Ptjet_Cut_5_SQG_Set2.eps">
    <img src="%ATTACHURL%/Ptjet_Cut_5_SQG_Set2.png"width=45% ></img></a>

<div style="width:80%;">
*Figure 9:* <i>Point2 selection results.</i> Reconstructed number of jets, %$N^{jet}$%, distributions after cuts 1,2,3,45, Section 7, in %$A$% (top left) and (%$\tilde{q},\tilde{g}$%) (bottom right) events. All distributions are normalized at %$\int\mathcal{L} = 300 fb^{-1}$%. Bin width = 1 !GeV.
</div>
</div>

<div align="center" style="width:800px">
<a href="%ATTACHURL%/Set1_sf5_tb_vs_MA_300fb_pap.eps">
    <img src="%ATTACHURL%/Set1_sf5_tb_vs_MA_300fb_pap.png"width=45% ></img></a>
<a href="%ATTACHURL%/Set1_sf2_tb_vs_MA_300fb_pap.eps">
    <img src="%ATTACHURL%/Set1_sf2_tb_vs_MA_300fb_pap.png"width=45% ></img></a>
<a href="%ATTACHURL%/Set1_sf5_tb_vs_MA_100fb_pap.eps">
    <img src="%ATTACHURL%/Set1_sf5_tb_vs_MA_100fb_pap.png"width=45% ></img></a>
<a href="%ATTACHURL%/Set1_sf2_tb_vs_MA_100fb_pap.eps">
    <img src="%ATTACHURL%/Set1_sf2_tb_vs_MA_100fb_pap.png"width=45% ></img></a>

<div style="width:80%;">
*Figure 10:* <i>Set1</i>. Discovery potential for a neutral Higgs boson %$A/H$% of mass %$m_A$% decaying to four leptons accompanied by missing transverse energy, as a function of %$m_A$%: contours are drawn for a search significance %$\frac{S}{\sqrt{B}}=5$% (left) and %$\frac{S}{\sqrt{B}}=2$% (right), with an integrated luminosity of %$\int\mathcal{L} = 300 fb^{-1}$% (top) and %$100 fb^{-1}$% (bottom). No discovery region is found for this latter luminosity. %$S$% is the number of signal events, %$B$% is the number of background events.
</div>
</div>


<div align="center" style="width:800px">
<a href="%ATTACHURL%/Set2_sf5_tb_vs_MA_300fb_pap.eps">
    <img src="%ATTACHURL%/Set2_sf5_tb_vs_MA_300fb_pap.png"width=45% ></img></a>
<a href="%ATTACHURL%/Set2_sf2_tb_vs_MA_300fb_pap.eps">
    <img src="%ATTACHURL%/Set2_sf2_tb_vs_MA_300fb_pap.png"width=45% ></img></a>
<a href="%ATTACHURL%/Set2_sf5_tb_vs_MA_100fb_pap.eps">
    <img src="%ATTACHURL%/Set2_sf5_tb_vs_MA_100fb_pap.png"width=45% ></img></a>
<a href="%ATTACHURL%/Set2_sf2_tb_vs_MA_100fb_pap.eps">
    <img src="%ATTACHURL%/Set2_sf2_tb_vs_MA_100fb_pap.png"width=45% ></img></a>

<div style="width:80%;">
*Figure 11:* <i>Set2</i>. Discovery potential for a neutral Higgs boson %$A/H$% of mass %$m_A$% decaying to four leptons accompanied by missing transverse energy, as a function of %$m_A$%: contours are drawn for a search significance %$\frac{S}{\sqrt{B}}=5$% (left) and %$\frac{S}{\sqrt{B}}=2$% (right), with an integrated luminosity of %$\int\mathcal{L} = 300 fb^{-1}$% (top) and %$100 fb^{-1}$% (bottom). %$S$% is the number of signal events, %$B$% is the number of background events.
</div>
</div>

<div align="center" style="width:800px">
<a href="%ATTACHURL%/Set2_tH_sf5_tb_vs_MA_300fb_pap.eps">
    <img src="%ATTACHURL%/Set2_tH_sf5_tb_vs_MA_300fb_pap.png"width=45% ></img></a>
<a href="%ATTACHURL%/Set2_tH_sf2_tb_vs_MA_300fb_pap.eps">
    <img src="%ATTACHURL%/Set2_tH_sf2_tb_vs_MA_300fb_pap.png"width=45% ></img></a>
<a href="%ATTACHURL%/Set2_tH_sf5_tb_vs_MA_100fb_pap.eps">
    <img src="%ATTACHURL%/Set2_tH_sf5_tb_vs_MA_100fb_pap.png"width=45% ></img></a>
<a href="%ATTACHURL%/Set2_tH_sf2_tb_vs_MA_100fb_pap.eps">
    <img src="%ATTACHURL%/Set2_tH_sf2_tb_vs_MA_100fb_pap.png"width=45% ></img></a>

<div style="width:80%;">
*Figure 12:* <i>Set2 including %$H^{\pm}$%</i>. Discovery potential for a Higgs boson %$A/H/H^{\pm}$% of mass %$m_A$% decaying to four leptons accompanied by missing transverse energy, as a function of %$m_A$%: contours are drawn for a search significance %$\frac{S}{\sqrt{B}}=5$% (left) and %$\frac{S}{\sqrt{B}}=2$% (right), with an integrated luminosity of %$\int\mathcal{L} = 300 fb^{-1}$% (top) and %$100 fb^{-1}$% (bottom). %$S$% is the number of signal events, %$B$% is the number of background events.
</div>
</div>

<div align="center" style="width:800px">
<a href="%ATTACHURL%/Significance_SetA_pap.eps">
    <img src="%ATTACHURL%/Significance_SetA_pap.png"width=45% ></img></a>
<a href="%ATTACHURL%/Significance_SetB_pap.eps">
    <img src="%ATTACHURL%/Significance_SetB_pap.png"width=45% ></img></a>

<div style="width:80%;">
*Figure 13:* <i>SetA, !SetB</i>. Discovery potential for a Higgs boson %$A/H$% of mass %$m_A$% decaying to four leptons accompanied by missing transverse energy,  as a function of %$m_A$%, for mSUGRA !SetA (right) and !SetB (left): values of the search significance, %$\frac{S}{\sqrt{B}}$%, with an integrated luminosity of %$\int\mathcal{L} = 300 fb^{-1}$% (blue bulet) and %$100 fb^{-1}$% (red triangle). The blue and green lines correspond to a search significance %$\frac{S}{\sqrt{B}}=5$% and %$\frac{S}{\sqrt{B}}=2$%, respectively. %$S$% is the number of signal events, %$B$% is the number of background events.
</div>
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*Major updates*:%BR%
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Topic revision: r5 - 2011-01-26 - PatrickJussel
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