Measurement of the correlated b-bbar production in p-pbar collisions at 1960 GeV
We present a measurement of the correlated bb
production cross section. The data used in this analysis were taken with the upgraded
CDF (CDF II) detector at the Fermilab Tevatron collider, and correspond to an
integrated luminosity of 742 pb-1. We utilize muon pairs with invariant
mass 5 &le m&mu&mu &le 80 GeV/c2
produced by bb double semileptonic
decays. For muons with pT &ge 3 GeV/c and |&eta| &le 0.7, which
in turn are produced by b and b quarks
with pT &ge 2 GeV/c and |y| &le 1.3, we measure
&sigmab&rarr&mu, b&rarr&mu
= 1549 ± 133 pb. We compare this result with theoretical predictions and previous
measurements. We also report the measurement of
&sigmac&rarr&mu, c&rarr&mu,
a by-product of the study of the background to bb production.
The results have been approved as of May 24, 2007.
A more detailed summary of the results can be found here: ps , pdf .
Below are the eps and gif versions of all figures meant for downloads.
- Figure : 1D impact parameter templates
(.eps) (.gif)
- Figure : m&mu&mu in the Upsilon region
(.eps) (.gif)
- Figure : 1D projection of some 2D templates used in the fit
(.eps) (.gif)
- Figure : 2D impact parameter distribution of &mu&mu pairs
(.eps) (.gif)
- Figure : m&mu&mu for all &mu&mu pairs used in this study
(.eps) (.gif)
- Figure : 1D projection of the 2D impact parameter fit (B/W)
(.eps) (.gif)
- Figure : Impact parameter distributions of kaons and pions from (a) b- and (b) c-quark decays
are compared to those of muons from semileptonic decays (MC).
(.eps) (.gif)
- Figure : 1D projection of the 2D impact parameter fit
(.eps) (.gif)
- Figure : Pulls of the 2D fit
(.eps) (.gif)
- Figure : pT data vs MC (bb)
(.eps) (.gif)
- Figure : pT data vs MC (cc)
(.eps) (.gif)
- Figure : &delta&phi&mu&mu data vs MC (bb)
(.eps) (.gif)
- Figure : &delta&phi&mu&mu data vs MC (cc)
(.eps) (.gif)
- Figure : m&mu&mu data vs MC (bb)
(.eps) (.gif)
- Figure : m&mu&mu data vs MC (cc)
(.eps) (.gif)
- Figure : prompt muons pT (data)
(.eps) (.gif)
- Figure : pT bb vs cc (MC)
(.eps) (.gif)
- Figure : m&mu&mu prompt sPlot (Upsilons zoom)
(.eps) (.gif)
- Figure : distribution of the event vertex along the beamline
(.eps) (.gif)
- Figure : D0 candidates
(.eps) (.gif)
- Figure : D* candidates
(.eps) (.gif)
- Figure : D0 candidates with fake &mu from K
(.eps) (.gif)
- Figure : D0 candidates with fake &mu from &pi
(.eps) (.gif)
- Figure : D0 candidates with fake &mu from K (&chi2CMU>9)
(.eps) (.gif)
- Figure : D0 candidates with fake &mu from K (&chi2CMU< 9)
(.eps) (.gif)
- Figure : D0 candidates with fake &mu from &pi (&chi2CMU>9)
(.eps) (.gif)
- Figure : D0 candidates with fake &mu from &pi (&chi2CMU< 9)
(.eps) (.gif)
- Figure : &mu from K fake rate vs pT
(.eps) (.gif)
- Figure : &mu from &pi fake rate vs pT
(.eps) (.gif)
- Figure : pT of K that can fake a &mu (data vs MC)
(.eps) (.gif)
- Figure : pT of &pi that can fake a &mu (data vs MC)
(.eps) (.gif)
- Figure : efficiency for a real &mu to pass the &chi2CMU< 9 cut
(.eps) (.gif)
- Figure : Silicon selection efficiency for 1st leg
(.eps) (.gif)
- Figure : Silicon selection efficiency for 2nd leg
(.eps) (.gif)
- Figure : CMUP selection efficiency
(.eps) (.gif)
- Figure : L1 trigger primitive efficiency
(.eps) (.gif)