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2011 QCD and High Energy Interactions - Rencontres de Moriond ...

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Table 1: Table listing the various channels <strong>and</strong> sub-channels inclu<strong>de</strong>d in the latest update to the combined Higgs<br />

searches from the Tevatron, indicating the integrated luminosity used <strong>and</strong> the mass range.<br />

Channel Sub channels Luminosity (fb−1 Contributing channels from CDF<br />

mH range (GeV)<br />

H→W + W− WH→WW<br />

2×(0,1 jets) + (2+ jets) + (low-mll) + (e-τhad)+(µ − τhad) 7.1 130-200<br />

+ W− (same-sign leptons 1+ jets) + (tri-leptons) 7.1 130-200<br />

ZH→ZW + W− (tri-leptons 1 jet) + (tri-leptons 2+ jets) 7.1 130-200<br />

Contributing channels from D0<br />

H→W + W− → l ± νl∓ν (0,1,2+ jets) 8.1 130-200<br />

H→W + W− → µντhadν 7.3 130-200<br />

H→W + W− → l¯νjj 5.4 130-200<br />

VH→ l ± l ± + X 5.3 130-200<br />

H+X→ l ± τ ∓<br />

jj had<br />

H→ γγ<br />

4.3<br />

8.2<br />

130-200<br />

130-150<br />

shown in a single figure. In the left panel, the light (pale-blue) sha<strong>de</strong>d histogram shows the<br />

background prediction, the dark (red) sha<strong>de</strong>d region shows the signal prediction for the a SM<br />

Higgs boson of mH = 165 GeV on top of the background prediction <strong>and</strong> the points show the<br />

observed data. Good agreement between data <strong>and</strong> background prediction is seen across several<br />

or<strong>de</strong>rs of magnitu<strong>de</strong> in s/b. The right h<strong>and</strong> panel of Figure 1 shows a zoomed-in region of the<br />

left-h<strong>and</strong> plot looking at the high s/b region. Here, the points show the data with the expected<br />

background subtracted, the sha<strong>de</strong>d histogram the predicted signal <strong>and</strong> the open histogram the<br />

approximate ± 1 st<strong>and</strong>ard <strong>de</strong>viation of the background prediction. Here it can clearly be seen<br />

that towards the right-h<strong>and</strong> edge of the plot the signal histogram rises above the uncertainties<br />

on the background mo<strong>de</strong>l.<br />

Events<br />

10 6<br />

10 5<br />

10 4<br />

10 3<br />

10 2<br />

10<br />

1<br />

10 -1<br />

10 -2<br />

10 -3<br />

Tevatron Run II Preliminary, L ≤ 8.2 fb -1<br />

m H =165 GeV/c 2<br />

Tevatron Data<br />

Background<br />

Signal<br />

March 7, <strong>2011</strong><br />

-4 -3 -2 -1 0 1<br />

log 10 (s/b)<br />

Events/0.13<br />

50<br />

40<br />

30<br />

20<br />

10<br />

0<br />

-10<br />

-20<br />

-30<br />

-40<br />

-50<br />

Tevatron Run II Preliminary<br />

L ≤ 8.2 fb -1<br />

Data-Background<br />

SM Higgs Signal<br />

±1 s.d. on Background<br />

March 7, <strong>2011</strong> m H =165 GeV/c 2<br />

-1.8 -1.6 -1.4 -1.2 -1 -0.8 -0.6 -0.4 -0.2 0<br />

log 10 (s/b)<br />

Figure 1: A comparison of the expected backgrounds (b) , signal (s) for a SM Higgs boson of mH = 165 GeV, <strong>and</strong><br />

data binned across all channels in log10(s/b). In the left panel the light sha<strong>de</strong>d region represents the expected<br />

backgrounds, the dark sha<strong>de</strong>d region the expected signal <strong>and</strong> the crosses are the data. In the right panel the<br />

expected background has been subtracted from the data. The solid histogram shows the expected signal, the<br />

points show the data <strong>and</strong> the open histogram shows the expected ±1 st<strong>and</strong>ard <strong>de</strong>viation of the background<br />

prediction.<br />

In or<strong>de</strong>r to ensure that the limits do not <strong>de</strong>pend strongly on the choice of statistical analysis,<br />

two approaches are consi<strong>de</strong>red making use of both Bayesian <strong>and</strong> modified frequentist methods.<br />

In both cases the full distributions of the final discriminants are used, not just the overall<br />

rates. Systematic uncertainties are taken into consi<strong>de</strong>ration on both the signal <strong>and</strong> background

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