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2 The CDF Experiment at Fermilab Contents - Harvard University ...

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Section 2: W Mass 61<br />

250<br />

200<br />

<strong>CDF</strong>(1B) Preliminary<br />

Z→ee χ 2 /df=1.3<br />

κ %<br />

2.25<br />

2<br />

1.75<br />

2σ<br />

1σ<br />

150<br />

1.5<br />

100<br />

1.25<br />

50<br />

1<br />

0<br />

70 80 90 100 110<br />

<strong>CDF</strong>(1B) Preliminary<br />

250<br />

Z→µµ χ 2 /df=0.89<br />

200<br />

150<br />

100<br />

50<br />

σ(1/p T<br />

)x10 -3 GeV -1<br />

1.05<br />

1<br />

0.95<br />

0.9<br />

0.85<br />

0.998 1 1.002<br />

Mz/Mz(LEP)<br />

2σ<br />

1σ<br />

0<br />

80 90 100<br />

0.8<br />

0.998 1 1.002<br />

Mz/Mz(LEP)<br />

Figure 31: Shown on the left is the Z mass in the muon and electron channels used for setting<br />

the energy scale of the calorimeter. On the right are plots of the resolution of the calorimeter<br />

or tracking chamber, versus the r<strong>at</strong>io of the tted Z mass to the LEP measured Z mass.

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