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

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Data / MC<br />

CMS preliminary, 2.9 pb<br />

1.1<br />

s = 7 TeV<br />

1.08<br />

MC scaled for FSR <strong>and</strong> <strong>QCD</strong> bkg<br />

pT balance<br />

1.06<br />

1.04<br />

1.02<br />

1<br />

0.98<br />

0.96<br />

anti-kT 0.5 PF<br />

MPF<br />

χ2<br />

/ NDF = 14.2 / 12<br />

20 30 40 50 100 200<br />

γ<br />

p (GeV)<br />

-1<br />

T<br />

Absolute scale uncertainty [%]<br />

10<br />

9<br />

8<br />

7<br />

6<br />

5<br />

4<br />

3<br />

2<br />

1<br />

0<br />

-1<br />

CMS preliminary, 2.9 pb<br />

particle flow jets<br />

Anti-k 0.5 & 0.7<br />

T<br />

Total uncert.<br />

Total MPF<br />

Photon scale<br />

Extrapolation<br />

Offset (+1PU)<br />

Residuals<br />

s = 7 TeV<br />

20 30 100 200 1000 2000<br />

p (GeV)<br />

Figure 1: Left: Ratio between measured jet absolute energy scale with photon+jet events <strong>and</strong> the one predicted<br />

by the MC simulation, as a function of photon pT. Results obtained with the Missing-ET Projection Fraction<br />

(MPF) method (red) are compared to a traditional photon/jet balancing technique (blue). Right: Uncertainty<br />

on the absolute scale measurement with the MPF method. Different sources of error are shown.<br />

• an absolute correction, which addresses the non-compensating nature of the CMS calorimeters,<br />

<strong>and</strong> uniforms the response as a function of jet transverse momentum.<br />

The measurement of the relative <strong>and</strong> absolute corrections has been performed on the first<br />

3 pb −1 of data recor<strong>de</strong>r in 2010. The jet absolute correction is measured on photon+jet events,<br />

in which the precision with which the photon is reconstructed in the crystal electromagnetic<br />

calorimeter is exploited in or<strong>de</strong>r to infer the recoiling jet’s true momentum. The absolute<br />

response is extracted making use of the knowledge of the full event missing transverse energy,<br />

with a method know as the Missing-ET Projection Fraction (MPF) 2 . This method is particularly<br />

suited for the Particle-Flow event reconstruction, which, through the use of the tracker, ensures<br />

a relatively high response also in the case of soft radiation. It is therefore expected to be the<br />

most insensitive to biases related to additional event activity.<br />

Results obtained with the photon+jet pt balancing technique are shown in Fig. 1 (left),<br />

where the MPF data/MC ratio (blue) is shown as a function of the photon transverse momentum.<br />

Results obtained with a more traditional photon/jet balancing technique are shown as<br />

comparison (red). The points are compatible with the Monte Carlo prediction. The estimated<br />

systematic uncertainty on this measurement is shown in Fig. 1 (right). Various possible sources<br />

resolution<br />

T<br />

jet p<br />

0.3<br />

0.2<br />

0.1<br />

-1<br />

s=7 TeV, L=35.9 pb CMS preliminary 2010<br />

total systematic uncertainty<br />

MC truth (c-term ad<strong>de</strong>d)<br />

MC truth<br />

data<br />

0<br />

50 100 200<br />

CaloJets<br />

(Anti-k R=0.5)<br />

T<br />

0 < | η|<br />

≤ 0.5<br />

p [GeV]<br />

T<br />

resolution<br />

T<br />

jet p<br />

0.3<br />

0.2<br />

0.1<br />

total systematic uncertainty<br />

MC truth (c-term ad<strong>de</strong>d)<br />

MC truth<br />

data<br />

0<br />

50 100 200<br />

T<br />

-1<br />

s=7 TeV, L=35.9 pb CMS preliminary 2010<br />

PFJets<br />

(Anti-k R=0.5)<br />

T<br />

0 < | η|<br />

≤ 0.5<br />

p [GeV]<br />

T<br />

Figure 2: Jet transverse momentum resolution measurement with the dijet asymmetry method in the central part<br />

of the <strong>de</strong>tector (|η| < 0.5). Calorimeter jet results are shown on the left, Particle-Flow jets on the right.

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