Difference: PublicPlotsHG10 (1 vs. 14)

Revision 142011-01-26 - PatrickJussel

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META TOPICPARENT name="Atlas.PhysicsResults"
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Please modify it in the sections indicated to create your topic! In particular, notice that at the bottom there are some sections that must be filled for publicly accessible pages.
If you have any comments/complaints about this template, then please email : Stephen Haywood (Computing Documentation Coordinator)
S.Haywood at rl.ac.uk (or failing that, edward.moyse at cern.ch)
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Charged Higgs boson searches

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Revision 132010-12-20 - PeterJones

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Revision 122009-12-01 - CalebLeeParnellLampenExCern

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META TOPICPARENT name="PhysicsResults"
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Charged Higgs boson searches

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Responsible: CalebLampen
 
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Revision 112009-04-15 - WolfgangMader

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META TOPICPARENT name="PhysicsResults"
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Changed:
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<
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Revision 102009-02-05 - WolfgangMader

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META TOPICPARENT name="PhysicsResults"
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<
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  • Set ALLOWTOPICCHANGE=WolfgangMader,AleandroNisati,KeteviAssamagan,BillMurray,WilliamMurray,DaveCharlton,TomLeCompte
 
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Revision 92009-02-05 - WolfgangMader

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META TOPICPARENT name="PhysicsResults"
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Charged Higgs boson searches (HG10)

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Charged Higgs boson searches

 
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 82009-02-02 - WolfgangMader

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META TOPICPARENT name="PhysicsResults"
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  • Set ALLOWTOPICCHANGE=WolfgangMader
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Revision 72009-01-30 - WolfgangMader

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META TOPICPARENT name="PhysicsResults"
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Charged Higgs boson searches (HG10)

 
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Additional Approved Plots

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Revision 62009-01-29 - WolfgangMader

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META TOPICPARENT name="PhysicsResults"
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Caption: tt->bH+ bW->bτ(had)νbqq: Likelihood distribution (a) and transverse mass (b) for an H+ mass of 130 GeV and the corresponding background, stacked and normalized to the cross-section with tanβ=20. The hatched area shows what would be expected from a Standard Model only scenario. A cut at 0.6 is made on the likelihood and at 65 GeV on the transverse mass.
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Figure 1: tt->bH+ bW->bτ(had)νbqq: Likelihood distribution (a) and transverse mass (b) for an H+ mass of 130 GeV and the corresponding background, stacked and normalized to the cross-section with tanβ=20. The hatched area shows what would be expected from a Standard Model only scenario. A cut at 0.6 is made on the likelihood and at 65 GeV on the transverse mass.
 

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Caption: tt->bH+bW->bτ(had)νbqq: Discovery (left) and exclusion contour (right) for Scenario B (mh -max) [1]. Systematic and statistical uncertainties are included. The systematic uncertainty is assumed to be 10% for the background, and 24% for the signal (see Sections 5.2 and 5.1). The lines indicate a 5σ significance for the discovery and a 95% CL for the exclusion contour.
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Figure 2: tt->bH+bW->bτ(had)νbqq: Discovery (left) and exclusion contour (right) for Scenario B (mhmax). Systematic and statistical uncertainties are included. The systematic uncertainty is assumed to be 10% for the background, and 24% for the signal (see Sections 5.2 and 5.1). The lines indicate a 5σ significance for the discovery and a 95% CL for the exclusion contour.
 

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Caption: tt->bH+bW->bτ(lep)νbqq: (a) cosφ distribution, (b) W transverse mass distribution, for signal and background, after selection cuts, for charged Higgs boson masses of 90 and 150 GeV.
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Figure 3: tt->bH+bW->bτ(lep)νbqq: (a) cosφ distribution, (b) W transverse mass distribution, for signal and background, after selection cuts, for charged Higgs boson masses of 90 and 150 GeV.
 

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Caption: tt->bH+bW->bτ(lep)νbqq: mh distribution, after selection cuts, for mTH<sup+ = 90, 120, and 150 GeV. The dotted line represents the nominal simulated mass.
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Figure 4: tt->bH+bW->bτ(lep)νbqq: mh distribution, after selection cuts, for mTH+=90, 120, and 150 GeV. The dotted line represents the nominal simulated mass.
 

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Figure 5: tt->bH+bW->bτ(lep)νbqq: Transverse mass differential cross-section for signal and background, for tanβ=20, and for the hypothesis of (a) W, and (b) H+.
 

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Figure 6: tt->bH+bW->bτ(lep)νbqq: Discovery (left) and exclusion contour (right) for Scenario B (mhmax). Systematic and statistical uncertainties are included. The systematic uncertainty is assumed to be 10% for the background, and 35% for the signal (see Sections 5.2 and 5.1). The lines indicate a 5σ significance for the discovery and a 95% CL for the exclusion contour.
 

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Figure 8: tt->bH+bW->bτ(had)νblν: ETmiss differential cross-section after all cuts for tanβ=20. The signal contributions for the different mass hypothesis are individually stacked on top of the background distribution.
 

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Caption: tt->bH+bW->bτ(had)νblν: Discovery (left) and exclusion contour (right) for Scenario B (mh -max) [1]. Systematic and statistical uncertainties are included. The systematic uncertainty is assumed to be 10% for the background, and 41% for the signal (see Sections 5.2 and 5.1). The lines indicate a 5σ significance for the discovery and a 95% CL for the exclusion contour.
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Figure 9: tt->bH+bW->bτ(had)νblν: Discovery (left) and exclusion contour (right) for Scenario B (mhmax). Systematic and statistical uncertainties are included. The systematic uncertainty is assumed to be 10% for the background, and 41% for the signal (see Sections 5.2 and 5.1). The lines indicate a 5σ significance for the discovery and a 95% CL for the exclusion contour.
 

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Caption: gg/gb -> t[b]H+ -> bqq[b]τ(had)ν: Probability density functions for tt and two signal mass points. The plots show, from the upper left to the lower right, log(pτT), log (ETmiss), and 1-cos(Δφ).
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Figure 10: gg/gb -> t[b]H+ -> bqq[b]τ(had)ν: Probability density functions for tt and two signal mass points. The plots show, from the upper left to the lower right, log(pτT), log (ETmiss), and 1-cos(Δφ).
 

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Caption: gg/gb -> t[b]H+ -> bqq[b]τ(had)ν: Likelihood distributions. The areas are normalized to unity. The background likelihood for 170 GeV does not peak at 0 because of the trigger selection (and to a smaller degree the less stringent preselection cuts for the PDF determination) which already removes most of the events in the first bins.
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Figure 11: gg/gb -> t[b]H+ -> bqq[b]τ(had)ν: Likelihood distributions. The areas are normalized to unity. The background likelihood for 170 GeV does not peak at 0 because of the trigger selection (and to a smaller degree the less stringent preselection cuts for the PDF determination) which already removes most of the events in the first bins.
 

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Figure 12: gg/gb -> t[b]H+ -> bqq[b]τ(had)ν: H+ transverse mass distributions for three signal mass points and the corresponding background for tanβ=35. The signal events are stacked on top of the background events.
 

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Caption: gg/gb -> t[b]H+ -> bqq[b]τ(had)ν: Discovery (left) and exclusion contour (right) for Scenario B (mh -max) [1]. Systematic and statistical uncertainties are included. The systematic uncertainty is assumed to be 10% for the background, and 44% for the signal (see Sections 5.2 and 5.1). The lines indicate a 5σ significance for the discovery and a 95% CL for the exclusion contour.
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Figure 13: gg/gb -> t[b]H+ -> bqq[b]τ(had)ν: Discovery (left) and exclusion contour (right) for Scenario B (mhmax). Systematic and statistical uncertainties are included. The systematic uncertainty is assumed to be 10% for the background, and 44% for the signal (see Sections 5.2 and 5.1). The lines indicate a 5σ significance for the discovery and a 95% CL for the exclusion contour.
 

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Caption: gg/gb -> t[b]H+ -> t[b]tb -> bW [b]bW b -> blν[b]bqqb: Reconstructed H+ mass. The value of tanβ has been chosen such that the pure statistical significance results in a value of 5.
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Figure 14: gg/gb -> t[b]H+ -> t[b]tb -> bW [b]bW b -> blν[b]bqqb: Reconstructed H+ mass. The value of tanβ has been chosen such that the pure statistical significance results in a value of 5.
 

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Figure 15: tt -> bτ(lep)νbqq: Left: W -> τ(lep)ν transverse mass, both for the real and the scaled tt events. Right: The corresponding bin-by-bin ratio. The gray band represents +/-10% around a ratio of 1.
 

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Figure 16: tt -> bτ(had)νbqq: Left: t -> bτ(had)ν momentum, both for the real and the scaled tt events. Right: The corresponding bin-by-bin ratio. The gray band represents +/-10% around a ratio of 1.
 

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Caption: Scenario A: Combined Results. Left: Discovery contour, Right: Exclusion contour. Systematic and statistical uncertainties are included.
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Figure 17: Scenario A: Combined Results. Left: Discovery contour, Right: Exclusion contour. Systematic and statistical uncertainties are included.
 

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Figure 18: Scenario B (mhmax): Combined Results. Left: Discovery contour, Right: Exclusion contour. Systematic and statistical uncertainties are included.
 

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Figure 19: Scenario B (mhmax): Combined Results. Left: Discovery contour, Right: Exclusion contour. Statistical errors arising from simulation statistics are neglected.
 

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Caption: Model-independent: Combined light H+ results in the (mH+, BR(t -> H+ b))-plane. Left: Discovery contour, Right: Exclusion contour. Systematic uncertainties and statistical uncertainties are included. BR(H+ -> τν) = 1 is assumed.
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Figure 20: Model-independent: Combined light H+ results in the (mH+, BR(t -> H+ b))-plane. Left: Discovery contour, Right: Exclusion contour. Systematic uncertainties and statistical uncertainties are included. BR(H+ -> τν) = 1 is assumed.
 

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Caption: Model-independent: Heavy H+ results in the (mH+, σ )-plane. Left: Discovery contour, Right: Exclusion contour. Systematic uncertainties and statistical uncertainties are included.
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Figure 21: Model-independent: Heavy H+ results in the (mH+, σ )-plane. Left: Discovery contour, Right: Exclusion contour. Systematic uncertainties and statistical uncertainties are included.
 

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Revision 52009-01-29 - WolfgangMader

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Revision 22009-01-28 - WolfgangMader

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Caption: tt->bH+bW->bτ(had)νbqq: Discovery (left) and exclusion contour (right) for Scenario B (mh -max) [1]. Systematic and statistical uncertainties are included. The systematic uncertainty is assumed to be 10% for the background, and 24% for the signal (see Sections 5.2 and 5.1). The lines indicate a 5σ significance for the discovery and a 95% CL for the exclusion contour.
 

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Caption: tt->bH+bW->bτ(lep)νbqq: (a) cosφ distribution, (b) W transverse mass distribution, for signal and background, after selection cuts, for charged Higgs boson masses of 90 and 150 GeV.
 

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< Caption: tt->bH+bW->bτ(lep)νbqq: Discovery (left) and exclusion contour (right) for Scenario B (mh -max) [1]. Systematic and statistical uncertainties are included. The systematic uncertainty is assumed to be 10% for the background, and 35% for the signal (see Sections 5.2 and 5.1). The lines indicate a 5σ significance for the discovery and a 95% CL for the exclusion contour.
 

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Caption: tt->bH+bW->bτ(had)νblν: (a) Multiplicity of jets and (b) τ jet transverse momentum (pτT).
 

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Caption: tt->bH+bW->bτ(had)νblν: ETmiss differential cross-section after all cuts for tanβ=20. The signal contributions for the different mass hypothesis are individually stacked on top of the background distribution.
 

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Caption: tt->bH+bW->bτ(had)νblν: Discovery (left) and exclusion contour (right) for Scenario B (mh -max) [1]. Systematic and statistical uncertainties are included. The systematic uncertainty is assumed to be 10% for the background, and 41% for the signal (see Sections 5.2 and 5.1). The lines indicate a 5σ significance for the discovery and a 95% CL for the exclusion contour.
 

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Caption: gg/gb -> t[b]H+ -> bqq[b]τ(had)ν: Probability density functions for tt and two signal mass points. The plots show, from the upper left to the lower right, log(pτT), log (ETmiss), and 1-cos(Δφ).
 

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Caption: gg/gb -> t[b]H+ -> bqq[b]τ(had)ν: Likelihood distributions. The areas are normalized to unity. The background likelihood for 170 GeV does not peak at 0 because of the trigger selection (and to a smaller degree the less stringent preselection cuts for the PDF determination) which already removes most of the events in the first bins.
 

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Caption: gg/gb -> t[b]H+ -> bqq[b]τ(had)ν: H+ transverse mass distributions for three signal mass points and the corresponding background for tanβ=35. The signal events are stacked on top of the background events.
 

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Caption: gg/gb -> t[b]H+ -> bqq[b]τ(had)ν: Discovery (left) and exclusion contour (right) for Scenario B (mh -max) [1]. Systematic and statistical uncertainties are included. The systematic uncertainty is assumed to be 10% for the background, and 44% for the signal (see Sections 5.2 and 5.1). The lines indicate a 5σ significance for the discovery and a 95% CL for the exclusion contour.
 

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Caption: gg/gb -> t[b]H+ -> t[b]tb -> bW [b]bW b -> blν[b]bqqb: Reconstructed H+ mass. The value of tanβ has been chosen such that the pure statistical significance results in a value of 5.
 

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Caption: tt -> bτ(lep)νbqq: Left: W -> τ(lep)ν transverse mass, both for the real and the scaled tt events. Right: The corresponding bin-by-bin ratio. The gray band represents +/-10% around a ratio of 1.
 

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Caption: tt -> bτ(had)νbqq: Left: t -> bτ(had)ν momentum, both for the real and the scaled tt events. Right: The corresponding bin-by-bin ratio. The gray band represents +/-10% around a ratio of 1.
 

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Caption: Scenario A: Combined Results. Left: Discovery contour, Right: Exclusion contour. Systematic and statistical uncertainties are included.
 

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Caption: Scenario B (mh -max): Combined Results. Left: Discovery contour, Right: Exclusion contour. Systematic and statistical uncertainties are included.
 

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Caption: Scenario B (mh -max): Combined Results. Left: Discovery contour, Right: Exclusion contour. Statistical errors arising from simulation statistics are neglected.
 

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Caption: Model-independent: Combined light H+ results in the (mH+, BR(t -> H+ b))-plane. Left: Discovery contour, Right: Exclusion contour. Systematic uncertainties and statistical uncertainties are included. BR(H+ -> τν) = 1 is assumed.
 

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Caption: Model-independent: Heavy H+ results in the (mH+, σ )-plane. Left: Discovery contour, Right: Exclusion contour. Systematic uncertainties and statistical uncertainties are included.
 

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Additional Plots

 
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Caption: tt -> bτ(lep)νbqq: Left: Lepton transverse momentum, both for the real and the scaled tt events. Right: The corresponding bin-by-bin ratio. The gray band represents +/-10% around a ratio of 1.
 

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Caption: tt -> bτ(had)νblν: Left: Missing transverse energy, both for the real and the scaled t t events. Right: The corresponding bin-by-bin ratio. The gray band represents +/-10% around a ratio of 1.
 

Revision 12009-01-27 - WolfgangMader

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META TOPICPARENT name="PhysicsResults"
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