1 / 12

Update on D0 reco. using KFParticle

Update on D0 reco. using KFParticle. J. Bouchet (KSU). outline. Update plots shown for the D0 reco : run over 3k events on the thick production Slight changes in the codes : p T of tracks > 0.5 GeV/c (was .3 before) Number of silicon hits = 4 (was 3 before)

gcrafton
Télécharger la présentation

Update on D0 reco. using KFParticle

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Update on D0 reco. using KFParticle J. Bouchet (KSU)

  2. outline • Update plots shown for the D0 reco : run over 3k events on the thick production • Slight changes in the codes : • pT of tracks > 0.5 GeV/c (was .3 before) • Number of silicon hits = 4 (was 3 before) • Cut on |n|<2.5 for the PID (was 3 before)

  3. Decay length significance SL zoom • SL = decay length / error (decay length)

  4. Inv. Mass D0 • left : invariant mass K-π+ before cut on SL • right : invariant mass K-π+ after cut on SL > 5

  5. Cut study dca<200µm SL>5 SL>10 SL>15 • Change the SL and dca pair track cut • Fit is done with pol1 function ; signal and background are evaluated in 1.84<M< 1.92 dca<100µm

  6. summary • Significance Seff = S/√(S+B) ,where • B = counts evaluated with the pol1 function • S = counts after background contribution Signal (S) background

  7. Decay length vs SL • left : decay length vs mass ; right : decay length significance vs mass • it is interesting to see that a cut on Sl seems to remove more efficiently the background (even we see a small peak at the correct inv. Mass on the left plot)

  8. Single track cut • The next plots are for the kaon track candidate • I look at some quantities for • All tracks (left panel) • Tracks where I select SL >5 and DCA pair < 200 µm (which from the plot I’ve shown before seems to select good D0 candidates) (right panel) • The beta factor for the kaon is calculated using the kaon mass assumption

  9. DCA distribution • Good kaon candidates (right) show that a min DCA cut is needed • DCA/DCA distribution • DCA is taken from the covariance matrix of track • Good kaon candidates (right) show that a cut ST =DCA/DCA could be applied

  10. DCA vs. (1/momentum) (X legend on the plot is flase) • We see the separation = min DCA cut for good kaon candidates

  11. DCA product • The product is defined as DCAXYkaon x DCAXYpion • The cos () is the cosine of the angle formed by the vector joining the primary vertex and the secondary vertex and the D0 momentum vector • As it has been shown before, the good D0 candidates exhibit a strong negative product • There is also a correlation between dcaProduct<0 and cos() > .9

  12. Summary /to do • Applying the decay length significance as a cut looks promising • Can apply another cuts (on the track level) • To do : • Correlation of cuts : for example, make the S/B map of D0 as a function of (Sl,DCA pair track) • Look at the other decays , as increasing the statistic confirm my previous results (based on less # events)

More Related