Some New Results in Heavy Flavor Physics - PowerPoint PPT Presentation

1 / 27
About This Presentation
Title:

Some New Results in Heavy Flavor Physics

Description:

G.Borissov, Dzero Hot Topics, FPCP-2004. 2. Many new results in heavy flavors physics: ... G.Borissov, Dzero Hot Topics, FPCP-2004. 12. Bs Studies. Properties ... – PowerPoint PPT presentation

Number of Views:37
Avg rating:3.0/5.0
Slides: 28
Provided by: Guennadi4
Category:
Tags: flavor | heavy | new | physics | results

less

Transcript and Presenter's Notes

Title: Some New Results in Heavy Flavor Physics


1
Some New Results in Heavy Flavor Physics
  • G.Borissov, Lancaster University, UK
  • representing DØ Collaboration

2
Many new results in heavy flavors physics
  • Properties of top quark
  • Bs lifetime from Bs?J/? f
  • Br(Bs ? µµ-)
  • Bd oscillations
  • Signals in Bs ? µ ?Ds
  • ?b lifetime
  • B masses
  • Properties of X(3872)
  • Bc lifetime

in this talk
talk of A.Nomerotski
Thanks to excellent performance of Tevatron
accelerator and DØ detector
3
Tevatron Performance
  • Peak luminosity above 1?1032 cm-2sec-1 achieved
  • Reliable operation of accelerator in stores 120
    hours/week
  • Expected peak luminosity 3?1032 cm-2sec-1 by
    2007
  • delivered luminosity to each experiment 4-8 fb-1
    by the end of 2009

4
(No Transcript)
5
Integrated Luminosity
  • Almost 0.5 fb-1 recorded in DØ
  • Most of analyses use only 30-50 of this
    statistics
  • more events available ? big room for
    improvement.

6
Top quark Studies
Provide important constraints on the SM Higgs
mass and new physics contribution
7
Top Quark Mass Measurement
  • New statistics from Run II (160 pb-1)
  • 191 events with lepton 4 jets selected
  • 4 topological variables used to separate ttbar
    and Wjets background. They are combined into a
    single discriminant.

8
Measurement Methods
  • 4 Jets and W can be combined into 2 top quarks in
    12 possible ways
  • Two alternative measurement methods used
  • Template method
  • apply cut on discriminant
  • select best mass hypothesis among all jet
    permutations
  • Ideogram method
  • discriminant is used to compute the purity of
    ttbar candidate on event by event basis
  • use all jet permutations with weight depending on
    the ?2 of each combination hypothesis.

9
Top Quark Mass Results
  • Consistent preliminary results are obtained (160
    pb-1)
  • Leading systematic uncertainty is from ttbar
    modeling, can be improved in the futre
  • In addition, new result published (Nature (429),
    638 (2004)) using Run I data (single most precise
    mass measurement)

10
Br(t?Wb)/Br(t ?Wq)
  • This ratio should be close to 1 in the SM,
    assuming unitarity of CKM matrix
  • Should be verified experimentally
  • Measurement is performed using a double tagging
    technique with b-tagging applied to the t-tbar
    sample (lepton plus jets).

11
RBr(t?Wb)/Br(t ?Wq) Result
  • Two b-tagging methods are used
  • Counting signed impact parameter
  • Secondary vertex Tagger
  • Consistent preliminary results are obtained
  • This result is consistent with R1.

12
Bs Studies
  • Properties of Bs are not well known yet
  • This particle is not accessible at ?(4s)
  • Have many interesting features
  • Bs oscillation
  • Lifetime difference of CP-even and CP-odd state
  • CP violation very small in SM, thus can be
    sensitive to the new physics
  • Rare decays may be enhanced
  • Bs is abundantly produced at Tevatron and can be
    reconstructed in both semileptonic and exclusive
    decays

13
Bs lifetime measurement
  • In this measurement the decay Bs? J/? f is used
  • In parallel, the lifetime of Bd in Bd? J/? K is
    measured very similar topology
  • Simultaneous measurement of Bd and Bs lifetimes
    reduces systematics in t(Bs) / t(Bd) ratio
  • Important step towards measurement of lifetime
    difference of CP-even and CP-odd Bs states.

14
Signal selection
220 pb-1 of DØ Run II data used
ct/s(ct) gt 5
ct/s(ct) gt 5
15
Lifetime fit
Two dimensional unbinned likelihood fit is used
Systematic uncertainties
16
Bs Lifetime Results
(FNAL-PUB-04/225-E, submitted to PRL)
This result agrees with other measurements of
t(Bs)
Experiment t(Bs)
DØ, this measurement 1.4440.098-0.0900.020
CDF (Run II) prelim 1.369 0.1000.008-0.010
CDF(Run I) semileptonic 1.36 0.0900.06-0.05
ALEPH 1.47 0.14 0.08
DELPHI 1.420.14-0.13 0.03
OPAL 1.500.16-0.15 0.04
17
Search for Bs?µµ-
Standard Model prediction
Rare B decays to leptons have very small expected
branching rates in SM. They can be significantly
higher in different SM extensions.
Br(Bd?ll-) Br(Bs?ll-)
l e (3.42.3) 10-15 (8.03.5) 10-14
lµ (1.50.9) 10-10 (3.40.5) 10-9
lt (3.11.9) 10-8 (7.41.9) 10-7
Current 90CL limits
Example SO(10) symmetry breaking model
Br(Bd?ll-) Br(Bs?ll-)
l e lt 5.9 10-6 lt 5.4 10-5
lµ lt 1.5 10-7 lt5.8 10-7
lt lt 2.5 lt 5.0
Contours of constant Br(Bs?µµ-)
18
Data sample
  • DØ has very efficient di-muon triggers
  • Use data collected in 2002 - April 2004
  • Sample corresponds to 250 pb-1 integrated
    luminosity.

19
Event Preselection
About 38000 candidates remain after preselection
20
Discriminating Variables
  • Pointing angle angle between Bs momentum and
    direction from primary to secondary vertex
  • Transverse decay length significance LT/s(LT)
  • Isolation

21
Optimization Procedure
  • 80 pb-1 of data is used to optimize the
    selection
  • Signal band is defined as m(BsDØ) 180 MeV (90
    MeV is Bs?µµ- resolution in MC)
  • Signal distributions are taken from MC and
    background from side bands
  • Perform random grid search of 3 discriminating
    variables and maximize the sensitivity to the
    signal.
  • Signal region in data is kept as a black box,
    open it only after finalizing and fixing the
    selection procedure
  • Number of events in side bands is used to
    estimate the background for Bs?µµ-

22
Surviving Events
cut Signal MC exp. background Signal
Pointing angle 8016 57314 580
Decay length significance 3847 4.31.2 5
Isolation 3746 3.71.1 4
23
Normalization Channel
  • B?J/? K (J/? ?µµ-) is used for normalization
  • muon selection efficiency cancels in the ratio
  • Systematics from discriminating variables
    significantly reduced.

24
Systematic uncertainties
Br(Bs?µµ-) Result
This measurement Existing limit (CDF)
90 CL lt 3.810-7 lt 5.810-7
95 CL lt 4.610-7 lt 7.510-7
25
Preparing for Bs oscillations
  • Bs oscillation measurement very interesting and
    very difficult task
  • Requires both selection of Bs signal and tagging
    its initial state (b or bbar)
  • Currently DØ selects Bs in semileptonic decays
  • We also develop methods of Bs selection in
    hadronic decays

26
Initial State Tagging
  • Three different methods are developed
  • Opposite muon tagging
  • Opposite jet charge tagging
  • Same side tagging
  • Their performance is verified in data using Bd
    oscillation

Same side tagging result
Tagging e D eD2
opposite muon 0.05 0.46 0.010
Same side 0.75 0.12 0.010
Same side Jet charge 0.68 0.15 0.015
27
Conclusions
  • Many new results in heavy flavor physics are
    obtained by DØ collaboration
  • All of them are competitive or the worlds best
    measurements
  • DØ will continue research in this direction with
    the main emphasis on studies complementary to
    B-factories those, involving B hadron states
    not produced at the ?(4s).
Write a Comment
User Comments (0)
About PowerShow.com