Difference: PublicPlotsHG11 (1 vs. 15)

Revision 152011-01-26 - PatrickJussel

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META TOPICPARENT name="Atlas.PhysicsResults"
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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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Statistical combination of several important Standard Model Higgs boson searches

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Revision 142010-12-20 - PeterJones

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Revision 132009-12-01 - CalebLeeParnellLampenExCern

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META TOPICPARENT name="PhysicsResults"
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Statistical combination of several important Standard Model Higgs boson searches

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Revision 122009-04-15 - WolfgangMader

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META TOPICPARENT name="PhysicsResults"
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Revision 112009-02-05 - WolfgangMader

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

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META TOPICPARENT name="PhysicsResults"
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Statistical combination of several important Standard Model Higgs boson searches (HG11)

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Statistical combination of several important Standard Model 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 92009-02-02 - WolfgangMader

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META TOPICPARENT name="PhysicsResults"
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Revision 82009-01-30 - WolfgangMader

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META TOPICPARENT name="PhysicsResults"
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Statistical combination of several important Standard Model Higgs boson searches (HG11)

 
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Revision 72009-01-29 - WolfgangMader

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Caption: Illustration of the determination of the p-value of a hypothesized value of μ. The left-hand curve indicates the pdf of qμ for data generated with the same value of μ as was used to define the statistic qμ ; this is used to determine the p-value of μ, shown as the shaded region. The right-hand curve indicates the pdf of qμ for data generated with a different value of the strength parameter, μ'.
>
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Figure 1: Illustration of the determination of the p-value of a hypothesized value of μ. The left-hand curve indicates the pdf of qμ for data generated with the same value of μ as was used to define the statistic qμ ; this is used to determine the p-value of μ, shown as the shaded region. The right-hand curve indicates the pdf of qμ for data generated with a different value of the strength parameter, μ'.
 

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Figure 2: Illustration of the correspondence between the significance Z and a p-value.
 

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Caption: Scatterplot of μ^ versus -2 ln λ(μ ); (b) the distribution of μ^ (see text).
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Figure 3: Scatterplot of μ^ versus -2 ln λ(μ ); (b) the distribution of μ^ (see text).
 

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Caption: Distributions of -2 ln λ (μ ) for (a) μ^ > μ and (b) μ^ <= μ. The superimposed curves are chi-square distributions for one degree of freedom normalized to half the number of entries in the original distribution (see Fig. 3(a)).
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Figure 5: Distributions of -2 ln λ (μ ) for (a) μ^ > μ and (b) μ^ <= μ. The superimposed curves are chi-square distributions for one degree of freedom normalized to half the number of entries in the original distribution (see Fig. 3(a)).
 

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Figure 6: The distribution of the test statistic q0 (for H -> γγ ), under the null background only hypothesis, for mH = 120 GeV with an integrated luminosity of 2 (a) and 10 (b) fb-1. A ½ χ12 distribution is superimposed.
 

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Caption: The distribution of the test statistic q1 for μ^ <= 1 under the s + b hypothesis (for H -> γγ ), for mH = 120 GeV with an integrated luminosity of (a) 2 fb-1 and (b) 10 fb-1. A &frac12 χ12 distribution is superimposed.
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Figure 7: The distribution of the test statistic q1 for μ^ <= 1 under the s + b hypothesis (for H -> γγ ), for mH = 120 GeV with an integrated luminosity of (a) 2 fb-1 and (b) 10 fb-1. A &frac12 χ12 distribution is superimposed.
 

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Caption: The distribution of the test statistic q0 for H + 0 j -> WW + 0 j, under the background-only hypothesis, with the same fixed QCD WW shape parameters used at both the generator and the fit level, for mH = 150 GeV and for an integrated luminosity of 10 fb-1 (a) with the same shape parameters for event generation and fitting; (b) with altered shape parameters. A &frac12 χ12 distribution is superimposed.
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Figure 8: The distribution of the test statistic q0 for H + 0 j -> WW + 0 j, under the background-only hypothesis, with the same fixed QCD WW shape parameters used at both the generator and the fit level, for mH = 150 GeV and for an integrated luminosity of 10 fb-1 (a) with the same shape parameters for event generation and fitting; (b) with altered shape parameters. A &frac12 χ12 distribution is superimposed.
 

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Figure 9: The distribution of the test statistic q1 for μ^ <= 1 under the s + b hypothesis for H + 0 j -> WW + 0 j, for mH = 150 GeV with an integrated luminosity of (a) 2 fb-1 and (b) 10 fb-1. A χ12 distribution is superimposed.
 

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Caption: The distribution of the test statistic q0 (for H + 2 j -> WW + 2 j), under the null background only hypothesis, for mH = 150 GeV and for an integrated luminosity of 2 (a) and 10 (b) f b-1. A &frac12 χ12 distribution is superimposed.
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Figure 10: The distribution of the test statistic q0 (for H + 2 j -> WW + 2 j), under the null background only hypothesis, for mH = 150 GeV and for an integrated luminosity of 2 (a) and 10 (b) f b-1. A ½ χ12 distribution is superimposed.
 

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Figure 11: The distribution of the test statistic q1 for μ^ <= 1 under the s + b (μ = 1) hypothesis (for H + 2 j -> WW + 2 j), for mH = 150 GeV with an integrated luminosity of (a) 2 fb-1 and (b) 10 fb-1. A χ12 distribution is superimposed.
 

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Caption: The distribution of the test statistic q0 for H -> τ τ under the null background-only hypothesis, for mH = 130 GeV with an integrated luminosity of 2 (a) and 10 (b) fb-1. A &frac12 χ12 distribution is superimposed. Figures (c) and (d) show 1 - F(q0 ) where F(q0 ) is the corresponding cumulative distribution. The small excess of events at high q0 is statistically compatible with the expected curves, as can be seen by comparison with the dotted histograms that show the 68.3% central confidence intervals for p = 1 - F(q0 |0). The lower dotted line at 2.87 x 10-7 shows the 5σ discovery threshold.
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Figure 12: The distribution of the test statistic q0 for H -> τ τ under the null background-only hypothesis, for mH = 130 GeV with an integrated luminosity of 2 (a) and 10 (b) fb-1. A ½ χ12 distribution is superimposed. Figures (c) and (d) show 1 - F(q0 ) where F(q0 ) is the corresponding cumulative distribution. The small excess of events at high q0 is statistically compatible with the expected curves, as can be seen by comparison with the dotted histograms that show the 68.3% central confidence intervals for p = 1 - F(q0 |0). The lower dotted line at 2.87×10-7 shows the 5σ discovery threshold.
 

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Caption: The distribution of the test statistic q1 for μ^ <= 1 under the s + b hypothesis for H -> τ+ τ- , for mH = 130 GeV with an integrated luminosity of (a) 2 fb-1 (b) and 10 fb-1. A χ12 distribution is superimposed.
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Figure 13: The distribution of the test statistic q1 for μ^ <= 1 under the s + b hypothesis for H -> τ+ τ- , for mH = 130 GeV with an integrated luminosity of (a) 2 fb-1 (b) and 10 fb-1. A χ12 distribution is superimposed.
 

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Caption: The distribution of the test statistic q0 (for H -> 4l), under the null background only hypothesis, for mH = 200 GeV with an integrated luminosity of 2 (a) and 10 (b) fb-1. A &frac12 χ12 distribution is superimposed. Figures (c) and (d) show 1 - F(q0 ) where F(q0 ) is the corresponding cumulative distribution. The small excess of events at high q0 is statistically compatible with the expected curves, as can be seen by comparison with the dotted histograms showing the 68.3% central confidence intervals for p = 1 - F(q0 |0). The lower dotted line at 2.87 x 10-7 shows the 5σ discovery threshold.
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Figure 14: The distribution of the test statistic q0 (for H -> 4l), under the null background only hypothesis, for mH = 200 GeV with an integrated luminosity of 2 (a) and 10 (b) fb-1. A ½ χ12 distribution is superimposed. Figures (c) and (d) show 1 - F(q0 ) where F(q0 ) is the corresponding cumulative distribution. The small excess of events at high q0 is statistically compatible with the expected curves, as can be seen by comparison with the dotted histograms showing the 68.3% central confidence intervals for p = 1 - F(q0 |0). The lower dotted line at 2.87×10-7 shows the 5σ discovery threshold.
 

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Figure 15: The distribution of the test statistic q1 for μ^ <= 1 under the s + b hypothesis (for H -> 4l), for mH=200 GeV with an integrated luminosity of (a) 2 fb-1 and (b) 10 fb-1. A χ12 distribution is superimposed.
 

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Figure 16: The median discovery significance for the various channels and the combination with an integrated luminosity of 10 fb-1 for (a) the lower mass range (b) for masses up to 600 GeV.
 

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Caption: Significance contours for different Standard Model Higgs masses and integrated luminosities. The thick curve represents the 5σ discovery contour. The median significance is shown with a colour according to the legend. The hatched area below 2 fb-1 indicates the region where the approximations used in the combination are not accurate, although they are expected to be conservative.
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Figure 17: Significance contours for different Standard Model Higgs masses and integrated luminosities. The thick curve represents the 5σ discovery contour. The median significance is shown with a colour according to the legend. The hatched area below 2 fb-1 indicates the region where the approximations used in the combination are not accurate, although they are expected to be conservative.
 

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Figure 18: The median p-value obtained for excluding a Standard Model Higgs Boson for the various channels as well as the combination for (a) the lower mass range (b) for masses up to 600 GeV.
 

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Figure 19: The expected luminosity required to exclude a Higgs boson with a mass mH at a confidence level given by the corresponding colour. The hatched area below 2 fb-1 indicates the region where the approximations used in the combination are not accurate, although they are expected to be conservative.
 

Revision 62009-01-29 - WolfgangMader

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Caption: Illustration of the determination of the p-value of a hypothesized value of μ. The left-hand curve indicates the pdf of qμ for data generated with the same value of μ as was used to define the statistic qμ ; this is used to determine the p-value of μ, shown as the shaded region. The right-hand curve indicates the pdf of qμ for data generated with a different value of the strength parameter, μ'.
 

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Caption: Distributions of -2 ln λ (μ ) for (a) μ^ > μ and (b) μ^ <= μ. The superimposed curves are chi-square distributions for one degree of freedom normalized to half the number of entries in the original distribution (see Fig. 3(a)).
 

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Caption: The distribution of the test statistic q0 (for H + 2 j -> WW + 2 j), under the null background only hypothesis, for mH = 150 GeV and for an integrated luminosity of 2 (a) and 10 (b) f b-1. A &frac12 χ12 distribution is superimposed.
 

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Caption: The distribution of the test statistic q1 for μ^ <= 1 under the s + b (μ = 1) hypothesis (for H + 2 j -> WW + 2 j), for mH = 150 GeV with an integrated luminosity of (a) 2 fb-1 and (b) 10 fb-1. A χ12 distribution is superimposed.
 

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Caption: The distribution of the test statistic q0 for H -> τ τ under the null background-only hypothesis, for mH = 130 GeV with an integrated luminosity of 2 (a) and 10 (b) fb-1. A &frac12 χ12 distribution is superimposed. Figures (c) and (d) show 1 - F(q0 ) where F(q0 ) is the corresponding cumulative distribution. The small excess of events at high q0 is statistically compatible with the expected curves, as can be seen by comparison with the dotted histograms that show the 68.3% central confidence intervals for p = 1 - F(q0 |0). The lower dotted line at 2.87 x 10-7 shows the 5σ discovery threshold.
 

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Caption: The distribution of the test statistic q1 for μ^ <= 1 under the s + b hypothesis for H -> τ+ τ- , for mH = 130 GeV with an integrated luminosity of (a) 2 fb-1 (b) and 10 fb-1. A χ12 distribution is superimposed.
 

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Caption: The distribution of the test statistic q0 (for H -> 4l), under the null background only hypothesis, for mH = 200 GeV with an integrated luminosity of 2 (a) and 10 (b) fb-1. A &frac12 χ12 distribution is superimposed. Figures (c) and (d) show 1 - F(q0 ) where F(q0 ) is the corresponding cumulative distribution. The small excess of events at high q0 is statistically compatible with the expected curves, as can be seen by comparison with the dotted histograms showing the 68.3% central confidence intervals for p = 1 - F(q0 |0). The lower dotted line at 2.87 x 10-7 shows the 5σ discovery threshold.
 

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Caption: The distribution of the test statistic q1 for μ^ <= 1 under the s + b hypothesis (for H -> 4l), for mH=200 GeV with an integrated luminosity of (a) 2 fb-1 and (b) 10 fb-1. A χ12 distribution is superimposed.
 

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Caption: Significance contours for different Standard Model Higgs masses and integrated luminosities. The thick curve represents the 5σ discovery contour. The median significance is shown with a colour according to the legend. The hatched area below 2 fb-1 indicates the region where the approximations used in the combination are not accurate, although they are expected to be conservative.
 

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fig03-a. fig03-b.
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fig04-a. fig04-b.
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fig05-a. fig05-b.
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fig12-a. fig12-b. fig12-c. fig12-d.
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Revision 12009-01-27 - WolfgangMader

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