| ttbar Production Cross-Section Ratio and Limits on Non-Standard Model Deacys of Top | |
| Ken Bloom and Monica Tecchio | |
| University of Michigan |
| Winter 2004 results with ~125 pb^-1 |
|---|
| R&sigma = 1.45+0.83-0.55 |
| R&sigma > 0.46 at 95% CL |
| R&sigma < 4.45 at 95% CL |
| &beta < 0.46 at 95% CL |
| &beta' < 0.47 at 95% CL |
Measuring the ttbar cross section establishes that we can find top. But
how do we know that the "top" that we observe in the dilepton decay mode
is the same "top" that we observe in the lepton plus jets mode? If both
are top, they should have the same production cross section. Thus, we
measure R&sigma =
&sigmall/&sigmalj. In taking the ratio, we are careful to handle the small
statistics, and to cancel the systematic uncertainties that are
correlated between the two analyses.
In addition, the cross-section measurements assume that top decays with
standard-model branching fractions, e.g. there is virtually always a W in
the decay, which decays with its usual branching fractions. If this is
not true, then our measured value for
R&sigma would not be consistent
with unity. Thus, one can use R&sigma
to extract limits on non-standard branching fractions of top. These limits
are by necessity model-dependent. We use a simple model which does not
have any particular physics motivation, but should give a reasonable
estimate of the efficiency to detect the non-standard decay.
| Description | gif | eps |
|---|---|---|
| Probability distribution function for the ratio that we observe in the data. |
|
eps |
| Probability distribution for the ratio of lepton plus jets to dilepton acceptances. Red is if you fail to cancel uncertainties that are correlated between the two acceptance estimates, green is if you do cancel them. There is an obvious improvement if you do the cancellation (but with our current statistics, it has no impact on the result). |
|
eps |
| Expected lower limits on beta (branching fraction to an all-hadronic decaying top) as a function of integrated luminosity. See the note for a description of the models. |
|
eps |
| Expected lower limits on beta-prime (branching fraction to an all-leptonic decaying top) as a function of integrated luminosity. See the note for a description of the models. |
|
eps |