Title: Measurement of bBaryons with the CDF II Detector
1Measurement of b-Baryons with the CDF II Detector
Joachim Heuser (University of Karlsruhe) for the
CDF Collaboration
2Short Reminder b-Baryons
- b-baryon is system of one heavy b-quark and two
light quarks - Naming scheme as for light baryons, b replaces
s-quark - Status as of 2006 only ?b0 directly observed
- This talk ?b, ?b
?b lifetime result from CDF covered by M.Milnik
on Friday B meson results from CDF covered by
A.Gessler on Thursday
3Why Look for b-Baryons ?
- b-baryon interesting laboratory for understanding
non-perturbative QCD and potential models - heavy b-quark ? sizeable simplification in
theoretical description - basic model light diquark system qq surrounding
the heavy b-quark nucleus Q - coupling similar as in hydrogen/helium atom
- never bad to observe new states ?
4Expectations on ?b()
- light diquark system has isospin I1, spin j1
- isospin-triplet ?b , ?0b , ?-b (?0b singlet)
- diquark spin j1 can couple with b spin to J1/2
(?b) or J3/2 (?b) - Theory Predictions
5?b Search
Channel ?/-b ? ?b ?/- with ?b ? ?c ?-
and ?c ? p K- ? Search for resonances in
Qm(?b ?) m(?b) m(?)
?0b2800
6?b Event Selection
- exclude 0.03 lt Q lt 0.10 GeV region from signal
selection procedure (blinding) - optimize selection based on
- MC simulation for ? signal sample
- sidebands from data, containing only background
events - fix background contributions
7?b Results
Observation of four signal peaks, associated with
?/-b() Significance of the signals gt5.2? (4
peaks vs. only BG) each peak gt3? (except
?b) Submitted to PRL arXiv0706.3868
8?b Masses
Good agreement with predictions !
9What Do We Know About the ?b ?
- quark content (usb / dsb)
- mass from extrapolation of charm baryons
- m(?b) - m(?b) m(?c) - m(?c)
- ? m(?b) m(?b) 180 MeV 5.8 GeV
-
- decay properties dominated by b-quark (with
light quarks as spectators) - ? expect similarities to other weakly decaying
b-hadrons
10Decay of the ?-b
- Search in channel
- ?-b ? J/? ?-,
- with ?- ??0 ?-, ?0 ? p ?-
?- is charged, long-lived, particle ? can be
measured in silicon detector ? significantly
improves resolution ? improves background
suppression
11Selection Strategy
- Lifetime and energy released in decay similar
between - ?-b ? J/? ?- and B ? J/? K
- unbiased selection optimization on B ? J/? K
sample
Keep 50 signal, reject factor 500 of background
12Observation of the ?-b
- Apply obtained selection on sample .
m 5792.9 2.5 1.7 MeV 7.7 ? significance
Submitted to PRL arXiv0707.0589
13Comparison
- In agreement with simultaneous observation by D0
and theory predictions
14Summary Outlook
- CDF observed the ?-b baryon
- m(?-b) 5792.9 2.5 1.7 MeV
- arXiv0707.0589
- CDF observed the charged ?b() baryons
- arXiv0706.3868
- results in good agreement with theory
predictions - CDF working great, lets see what we can still
do in the future (e.g. ?b lifetime) !
15Backup
16CDF II Detector
- Excellent tracking due to silicon layers near
interaction point and large tracking volume - Very important dedicated triggers for data
selection
17?b Significance Determination
- Form likelihood ratios between different
hypotheses (e.g. compare see 4 peaks to see
only two) - Ratios relative to 4-peak-hypothesis
18?b Cuts
Selection cuts for ?b
Selection cuts for ?b
19?b Backgrounds
- 3 main sources of background
- Hadronization and underlying events
- Tracks from hadronization of the b-quark,
modelled by ?b PYTHIA MC - Physics background
- Misidentified B, studied by B PYTHIA MC sample
- Combinatorial background
- Studied from upper data sideband
20?b Significance Determination
- Assume uniform distribution of background in mass
- Search window of 800 MeV
- Width of observed signal 75 MeV
- Binomial Probability of
- observing gt 18 events within 75 MeV bin
- from total of 23 events within 800 MeV