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

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58 Section 2: CDF Physics Analysis Figure 28: Best t E/p distribution for W events. Top left and right: Best t E/p distribution for Monte Carlo (histogram) with data overlayed (crosses), on a linear and log scale. Bottom: the residuals of the top plot, data minus Monte Carlo. The errors on the bottom points are the statistical errors associated with the data. Summing the squares over the points divided by their errors gives 2 =dof = 1:15. The tracking resolution for the Monte Carlo has (1=P T )=:00085 GeV ,1 . For 8% of the events, however, we use a second resolution of (1=P T ) = :0026 GeV ,1 . This second resolution is needed to account for the low-end E/p tail.
Section 2: W Mass 59 Figure 29: The distribution of (U 1 ,)= 1 (top) and U 2 = 2 (bottom) for all the Z data, where the model parameters are used tocalculate , 1 , and 2 . Gaussian ts to the histograms are overlayed, and the means and widths of the ts are printed on the plots.
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1 2 The CDF Experiment at Fermilab
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Section 2: CDF 3 of Run I data. Rec
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Section 2: CDF Hardware Projects 5
Page 7 and 8: Section 2: Central Outer Tracker 7
Page 21 and 22: Section 2: DAQ for the Silicon Vert
Page 27 and 28: Section 2: Central Muon Extension 2
Page 33: Section 2: Central Muon Extension 3
Page 36 and 37: 36 Section 2: CDF 2.3 Run I Physics
Page 38 and 39: 38 Section 2: CDF Physics Analysis
Page 93 and 94: Section 2: B Mixing and CP Violatio
Page 95 and 96: Section 2: B Mixing and CP Violatio
Page 97 and 98: Section 2: CDF 97 multijet trigger
Page 99 and 100: Section 2: CDF 99 The Jet Pseudora
Page 101 and 102: Section 2: CDF 101 while the proble
Page 103 and 104: Section 2: CDF 103 Talks at Confere
Page 105 and 106: Section 2: CDF 105 References [1] T
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