15
ICHEP 2010 Paris France 22-28 July 2010 New Babar Results in FCNC Decays : Search for B + → K + t + t - Search for B 0 gg Kevin Flood Univ. of Wisconsin (representing the Babar Collaboration)

New Babar Results in FCNC Decays : Search for B + → K + t + t - Search for B 0 → gg

Embed Size (px)

DESCRIPTION

New Babar Results in FCNC Decays : Search for B + → K + t + t - Search for B 0 → gg. Kevin Flood Univ. of Wisconsin (representing the Babar Collaboration). Final Babar dataset 426 fb -1 @ Y (4S) N(BB) = (467.8 ± 5.2) x 10 6. J. Hewett, PRD 53:4964 (1996). Search for B + → K + t + t -. - PowerPoint PPT Presentation

Citation preview

Page 1: New Babar Results in FCNC Decays : Search for B + → K + t + t - Search for B 0 → gg

ICHEP 2010 Paris France 22-28 July 2010

New Babar Results in FCNC Decays:

Search for B+ → K+ t+ t-

Search for B0 → gg

Kevin FloodUniv. of Wisconsin

(representing the Babar Collaboration)

Page 2: New Babar Results in FCNC Decays : Search for B + → K + t + t - Search for B 0 → gg

2ICHEP 2010 Kevin Flood 22-28 July 2010

Final Babar dataset

426 fb-1 @ Y(4S)

N(BB) = (467.8 ± 5.2) x 106

Page 3: New Babar Results in FCNC Decays : Search for B + → K + t + t - Search for B 0 → gg

3ICHEP 2010 Kevin Flood 22-28 July 2010

Search for B+ → K+ t+ t-

SM non-SM

Xs t+t-

Xs e+e-

J. Hewett, PRD 53:4964 (1996)

• B→Xt+t- SM rate similar to B→Xl+l- (l=e,m) in the kinematic region accessible to all

• B+→K+t+t- ~50% of total inclusive rate• NMSSM rate enhancements could be

proportional to (Mt2/Mm

2) ~ 280q2 = di-leptonmass squared

Page 4: New Babar Results in FCNC Decays : Search for B + → K + t + t - Search for B 0 → gg

Search for B+ → K+ t+ t- Fully reco’d hadronic B

Signal

K+

τ+ ντ

νμ, νe

e +, μ+

D(*)0,+

ϒ(4S)

B+B- τ-

ντ

νμ, νe

e-, μ-

X

0% 20% 4o% 60% 80% 100%

e

a1 t others

2 0 t

reconstructed tau decays

• 2-4 neutrinos in signal final state• Backgrounds controlled by recon-

structing recoiling B- in many fully hadronic final states• B- → D(*)0,+ + X

• X = up to total of six p0,p+, KS, K+

• Tag efficiency < ~0.2%

non-reconstructed tau decays

mES [GeV/c2 ]

22BbeamES pEm

t

Ebeam = ½ e+e- energy

beamB EEE

DE [GeV ]

DataContinuum-MCTotal FitContinuum PDFCombinatoric FitHadronic Tag Events

DataComb.MC+Tag MCComb. MCTag MC+Corr.Comb.Sbnd.Corr.Comb.

Page 5: New Babar Results in FCNC Decays : Search for B + → K + t + t - Search for B 0 → gg

5

Search for B+ → K+ t+ t- : Signal Selection

• Continuum backgrounds are suppressed using |cosqT|, the cosine of the opening angle between the tag B thrust and the rest-of-the-event thrust• All signal-side event

selection is done subsequent to applying the |cosqT| selection

ICHEP 2010 Kevin Flood 22-28 July 2010

|cosqT| < 0.8

• Three charged tracks only• one particle ID K+

• 0.44 < p < 1.4 GeV/c• charge opposite Btag

• one neutralpair of PID e, ,m p• p < 1.59 GeV/c• Mpair < 2.89 GeV/c2

• q2 = (pY4S - ptag - pK)2 > 14.23 GeV2

• Missing energy calculated from (pY4S – ptag – pK – pt1 – pt2 ) 4-vector• 1.39 < Emiss < 3.38 GeV

• Extra neutral energy < 0.74 GeV

• B→D+X decays are the largest remaining background, and are suppressed by combining the signal K+ with the signal tau daughter of opposite charge assigned a pion mass hypothesis and requiring the resulting invariant mass to be

• M(Kpi) > 1.96 GeV/c2

Signal MC

Continuum MC

Page 6: New Babar Results in FCNC Decays : Search for B + → K + t + t - Search for B 0 → gg

ICHEP 2010 Kevin Flood

Search for B+ → K+ t+ t- : Systematics, Results

BF(B+ → K+t+t-) < 0.0033 (90% CL)

B countingTag EfficiencySignal Efficiency - 13.9% MC Statistics

Background Estimate - Correct Tags - 5.1% Particle ID

- Incorrect Tags - 14.8% Data, MC statistics

1.1%3.2%14.8%

5.2%

14.8%

Expected Bkgd: 64.7 +/- 7.3Data Events: 47

Babar Preliminary

Babar Preliminary

Page 7: New Babar Results in FCNC Decays : Search for B + → K + t + t - Search for B 0 → gg

7ICHEP 2010 Kevin Flood 22-28 July 2010

Search for B0 → gg

Page 8: New Babar Results in FCNC Decays : Search for B + → K + t + t - Search for B 0 → gg

8ICHEP 2010 Kevin Flood 22-28 July 2010

Search for B0 → gg : Motivation, Previous Results

Experiment BF (90% CL) Dataset Ref.

L3 < 1.9 x 10-5 2.95x106 (Z→had)

Acciarri et al. Phys. Lett. B, 363, 1995

BaBar < 1.7 x 10-6 19 fb-1 Aubert et al. PRL 87, 24, 2001

Belle < 6.1 x 10-7 104 fb-1 Villa et al. PRD 73, 2006

• B0 → gg is an “effective” FCNC decay which is suppressed by CKM and EM vertex factors compared to b → (s,d)g

• Bs,d0 → gg constrained by B->Xs,dg

• |Vtd/Vts| accessible in simple two-body non-hadronic final state

• SM BF ~ 3 x 10-8 [Bosch and Buchalla, JHEP 0208:054 (2002)]

Page 9: New Babar Results in FCNC Decays : Search for B + → K + t + t - Search for B 0 → gg

Search for B0 → gg : Strategy, Event SelectionSelection Value(s)

N Tracks / event ≥ 3

Total Event Energy < 15.0 GeV

Cluster Timing 150 ns window

N cluster crystals > 10

Cluster isolation > 25 cm

Cluster Lateral Moment

0.15 ≤ LAT ≤ 0.5

π0 Likelihood Ratio ≤ 0.84

η Likelihood Ratio ≤ 0.84

Neural Network ≥ 0.54

• Blind analysis

• High-energy gbackgrounds•p0, h vetos•Out-of-time photons

• Small peaking backgrounds characterized with MC

• ~1.2 signal region events

• Continuum rejection with neural network using 19 event shape inputs

• Signal yield extracted from a 2-d fit to mES and DE

log scale

Signal

Background

Page 10: New Babar Results in FCNC Decays : Search for B + → K + t + t - Search for B 0 → gg

10ICHEP 2010 Kevin Flood 22-28 July 2010

Search for B0 → gg : p0, h Vetos

• Signal candidate photons (g) are paired with lower energy photons (g’) in an event, and the pair’s invariant mass M(gg’) and the soft photon’s energy E(g’) are used to construct a likelihood ratio with 2-d correlated likelihoods for signal events and background events obtained from simulated event samples

LR p0 LR h

SignalBackground

Signal

Background

Page 11: New Babar Results in FCNC Decays : Search for B + → K + t + t - Search for B 0 → gg

11ICHEP 2010 Kevin Flood 22-28 July 2010

Search for B0 → gg : Fit Method• Signal yield is extracted using a two-dimensional unbinned extended

maximum likelihood fit in mES and ΔE

• Three components in fit

• (1) Signal: pdf shapes from simulated events, normalization floated

• (2) Combinatoric Background: shape and normalization floated

• (3) Peaking Background: pdf shape and normalization from simulated events

• All signal PDF parameters are fixed in the fit

• Peaking background shape and yield are fixed in the fit

2D Histogram PDF

Component mES DeltaE

Signal Crystal Ball Asym Gaussian

Continuum Bkg ARGUS Polynomial O(1)

Peaking Bkg

Page 12: New Babar Results in FCNC Decays : Search for B + → K + t + t - Search for B 0 → gg

12ICHEP 2010 Kevin Flood 22-28 July 2010

Search for B0 → gg : Data Fit

• Signal and combinatoric yields, and the slope of the combinatoric mES Argus PDF, are floated in the fit:

• N signal = 21.3 (+12.8,-11.8)• BF(B0 → gg) = (1.7 +/- 1.1) x 10-7

TotalCombSignal

TotalCombSignal

BabarPreliminary

BabarPreliminary

Page 13: New Babar Results in FCNC Decays : Search for B + → K + t + t - Search for B 0 → gg

13ICHEP 2010 Kevin Flood 22-28 July 2010

Search for B0 → gg : Systematics, UL

N signal = 21.3 (+12.8,-11.8) +/- 1.4

SystematicsGaussian Conv.

90% CL

BabarPreliminary

Page 14: New Babar Results in FCNC Decays : Search for B + → K + t + t - Search for B 0 → gg

B → K*l+l-: FL and AFB Results (349 fb-1, 390x106 BB)

Longitudinal K* polarization

Lepton forward-backward asymmetry

C7=-C7SM

C9C10=-C9C10

SM

AFB=-AFB

SM

SM

F

L

low s 0.35 0.16 0.04

F

L

high s 0.71 0.22

0.20 0.05

A

FB

low s 0.24 0.23

0.18 0.06

A

FB

high s 0.76 0.32

0.52 0.07

PRD 79, 031102 (2009)

C7=-C7SM

SM

14ICHEP 2010 Kevin Flood 22-28 July 2010

Page 15: New Babar Results in FCNC Decays : Search for B + → K + t + t - Search for B 0 → gg

15

Summary

• Two new Babar results shown• First limit on B+ → K+t+t-

• BF(B+ → K+ t+ t-) < 0.0033% (90% CL)• Improvement of B0 → gg upper limit by a factor of

two• BF(B0 → )<gg 3.2 x 10-7 (90% CL)

• Further progress in these modes only possible at a high-luminosity B Factory

• B+ → K+t+t- sensitive to LFV effects, NMSSM• B0 → gg can probe B meson QCD dynamics and

provides a clean way to access |Vtd/Vts|• B → K*l+l- currently being updated to full Babar

dataset• Results will be reported in a manner allowing

trivial combination with recent Belle and CDF results

ICHEP 2010 Kevin Flood 22-28 July 2010