22.07.2013 Views

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

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

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

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

in for the inclusive trijet event sample also belong to the same pTmax bin for the inclusive<br />

dijet event sample. Given the <strong>de</strong>finitions above for inclusive n-jet event samples, R 3/2(pT max)<br />

equals the conditional probability for an inclusive dijet event (at pT max) to contain a third jet<br />

with pT > pT min. The data is well <strong>de</strong>scribed by the SHERPA event generator (using <strong>de</strong>fault<br />

settings) with tree-level matrix elements for 2-, 3-, <strong>and</strong> 4-jet production. For the PYTHIA event<br />

generator, the results <strong>de</strong>pend strongly on the chosen parameter tune. Commonly used tunes<br />

(for both the angular-or<strong>de</strong>red <strong>and</strong> the pT -or<strong>de</strong>red parton shower), see Fig. 3, overshoot the<br />

measured ratios significantly over the whole pT max range for all pT min requirements.<br />

R 3/2 = σ 3-jet / σ 2-jet<br />

0.2<br />

0.15<br />

0.1<br />

0.05<br />

0<br />

L int = 0.7 fb -1<br />

p Tmin = 50 GeV<br />

100 200 300 500<br />

DØ preliminary<br />

p Tmin = 70 GeV<br />

100 200 300 500<br />

p Tmax (GeV)<br />

SHERPA<br />

PYTHIA:<br />

tune A<br />

tune DW<br />

tune BW<br />

p Tmin = 90 GeV<br />

100 200 300 500<br />

Figure 3: R3/2 ratio measured as a function of the leading jet pT max for different pT min requirements for the<br />

other jets. Predictions from SHERPA <strong>and</strong> PYTHIA (three tunes using the virtuality-or<strong>de</strong>red parton shower) are<br />

compared to the data.<br />

3 Study of Substructure of <strong>High</strong> pT Jets<br />

The study of high transverse momentum (pT ) massive jets provi<strong>de</strong>s an important test of p<strong>QCD</strong><br />

<strong>and</strong> gives insight into the parton showering mechanism. In addition, massive boosted jets compose<br />

an important background in searches for various new physics mo<strong>de</strong>ls, the Higgs boson, <strong>and</strong><br />

highly boosted top quark pair production. Particularly relevant is the case where the <strong>de</strong>cay<br />

]<br />

2<br />

[1/GeV/c<br />

dNjet<br />

jet<br />

dm<br />

1<br />

Njet<br />

0.007<br />

0.006<br />

0.005<br />

0.004<br />

0.003<br />

0.002<br />

0.001<br />

Quark<br />

Gluon<br />

0.006<br />

0.004<br />

0.002<br />

0<br />

-1<br />

CDF Run II, L = 6 fb<br />

int<br />

Midpoint<br />

Anti-kT<br />

100 150 200 250<br />

Data, Midpoint, R = 0.7<br />

<strong>QCD</strong>, Pythia 6.216<br />

0<br />

80 100 120 140 160 180 200 220 240 260 280<br />

jet1 2<br />

m [GeV/c ]<br />

Figure 4: The normalized jet mass distribution for midpoint jets with pT > 400 GeV/c. The theory predictions<br />

for the jet functions for quarks <strong>and</strong> gluons are shown as solid curves <strong>and</strong> have an estimated uncertainty of 30%.<br />

The inset compares midpoint <strong>and</strong> anti − kt jets.<br />

of a heavy resonance produces high-pT top quarks that <strong>de</strong>cay hadronically. In all these cases,<br />

the hadronic <strong>de</strong>cay products can be <strong>de</strong>tected as a single jet with substructure that differs from

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!