Thomas Müller, Jeannine Wagner, Wolfgang Wagner
Abstract:
We present a measurement of the fraction of longitudinally
(F0) and right-handed (F+) polarized W bosons in top quark decays
using an integrated luminosity of about 320pb-1
collected at the CDF II detector. We are selecting ttbar events
with a lepton+jets signature in the detector.
For our helicity measurement we use the cosine of the decay angle &theta*
between the momentum of the charged lepton in the W boson rest frame and the W momentum
in the top quark rest frame, which is highly sensitive to the W helicity.
In order to determine the cos(&theta*) distribution in the data,
the kinematics of the ttbar events are fully reconstructed.
We find F0 = 0.85 +0.15 -0.22 (stat.) +- 0.06 (syst.) and
F+ = 0.05 +0.11 -0.05 (stat.) +- 0.03 (syst.),
which is well consistent with the standard model.
Final Results for 320 pb-1:
F0 = 0.85 +0.15 -0.22 (stat.) +- 0.06 (syst.)
F+ = 0.05 +0.11 -0.05 (stat.) +- 0.03 (syst.)
F+ < 0.26 at the 95% C.L.
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Introduction into W Helicity

Theoretical cos(&theta*) distribution (EPS)
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cos(&theta *) for longitudinally polarized W. (EPS)
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cos(&theta*) for left handed polarized W. (EPS)
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cos(&theta *) for right handed polarized W. (EPS)
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Measured cos(&theta*) Distribution

Measured cos(&theta*) distribution is shown together with the background estimate. (EPS)
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Measured cos(&theta *) distribution is shown together with the MC expectation. (EPS)
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Extraction of F0 and F+
F0 Extraction (F+=0)
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F+ Extraction (F0=0.7)
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Negative Likelihood function as a function of F0. The minimum represents the fit result. (EPS)
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Negative likelihood function as a function of F +. The minimum represents the fit result. (EPS)
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corrected cos(&theta*) distribution for data together with the
curve predicted for the fit result.
(EPS)
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corrected cos(&theta *) distribution for data together with the
curve predicted for the fit result.
(EPS)
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cos(&theta*) distribution for data together with the SM curve and
the curve predicted for the fit result.
(EPS)
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Statistical uncertainty

Distribution of the statistical uncertainty for pseudoexperiments. The statistical uncertainty of
our analysis is indicated by the arrow.
Systematic uncertainties:
Summary of systematic uncertainties, the total
error is calculated by adding all single uncertainties in quadrature.
Last modified: Wed May 24 04:03:31 CDT 2006
by T. Chwalek