Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional...

35
1 Study of B 0 X(3872) K + π - Anu Bala Jan 19, 2012

Transcript of Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional...

Page 1: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

1

Study of B0 →X(3872) K+ π-

Anu Bala

Jan 19, 2012

Page 2: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

2

Motivation

⧫ X(3872) not a conventional charmonium state

⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π signal, K* resonance has less

signal as compared to K π. Not compatible with: what is observed in

other charmonium decays like ψ' K+ π-.

⧫ Important to understand X(3872) nature and valuable for theoretical understanding of X(3872).

⧫ At present update/cross-check X(3872) K+ π- , later perform same study for the neutral decays.

Many thanks to Karim for giving this analysis as my Ph.D. topic.

Page 3: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

3

Introduction

Era of the new family of particles, named XYZ, started from the observation of X(3872) in the J/ψ π+π- final state by the Belle experimentMany new states have been found/observed/studied by Belle and other experiments, BaBar, CDF, D0, CLEO, CMS, LHC-b after that This is just a short list of them X(3872), X(3940), Y(3940), X(4160), Y(4008), Y(4260), Y(4350), Y(4660), Z(3930), Z(4415), Z(4430)+, Yb(10580), …These particles are not fittable to any of the known or predicted statesAngular analysis by CDF & Belle suggest its JPC to be 1++ or 2-+

Most probably it is new type of quark particles in addition to mesons and baryon, although it is not proved yet

Page 4: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

Observation of X(3872)

4

X(3872)Ψ '

M(π+π-l+l-)- M(l+l-) It did not fit to any known cc-bar statesMass of X(3872) is close to DD*

What is it: charmonium, DD*-molecule, tetraquark...?

Observed by Belle in B± → K± π+π-J/ψ 2003

Belle data: 152 M BB eventsMass = 3872.0±0.6±0.5 MeV/c2

Significance = 10 σNew Prediction of mass: Mass=3871.46±0.37±0.07 Mev/c2

152M BB, PRL91, 262001(2003)152M BB, PRL91, 262001(2003)

Page 5: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

Charmonium spectrum

Page 6: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

6

Selection criteria for X(3872) & Psi'B daughters selection:

charged particle selection: |dr|<1.0 cm & |dz|<2.8 cm Kid >0.6 πid>0.6 Pion of J/ψππ : πid>0.4 J/ψ reconstruction is done from leptonic mode Selection: 2.95 GeV/c2 < Me+e- <3.13 GeV/c2

: 3.02 GeV/c2 < Mμ+μ- <3.13GeV/c2

Mass constraint & vertex fit is applied. Bremsstrahlung photons within < 0.05 rad Momentum of J/ψ <1.8 GeV/c Mbc>5.27 GeV/c2 & |ΔE| <0.04 GeV Mπ+π- > 0.575 GeV/c2 & Mπ+π- > 0.389 GeV/c2

Will optimize ΔE cut500,000 events are generated for signal MC

Standard charmonium criteria used

Page 7: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

7

Reconstruction of J/ψ

J/ψ →μ+μ- J/ψ →e+e-

Mμμ GeV/c2

↓ ↓ ↓ ↓ Mee GeV/c2

Page 8: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

8

MKπ GeV/c2

BBψψ' K+ π-' K+ π-Bψ' K*0

BX(3872) K+ π-

MKπ distribution

BX(3872) K*0

MKπ GeV/c2

MKπ GeV/c2 MKπ GeV/c2

Page 9: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

9

Best Candidate Selection

*Estimated by performing fit to MJψππ

Decay Channel Multiplicity (%)

Reconstruction Efficiency* (%) Based on ΔE

Reconstruction efficiency* (%)Based on Mbc

B ψ' K+ π- 41.5 16.8 15.3

B ψ' K*(892) 40.4 16.1 14.9

B X(3872) K+π- 38.0 13.5 12.4

B X(3872) K*(892) 36.1 12.7 13.6

Tried selecting best candidate on basis of ΔE closest to 0 and Mbc closest to B nominal mass

Page 10: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

10Typical uncertainty on eff. , order of ~ 0.06%

Signal MC MJ/ψππ distribution

BBψψ' K+ ' K+ π-π-

Bψ' K*0

BX(3872) K+ π-

BX(3872) K*0

Eff= 16.1% Eff= 16.8%

Eff= 12.7%Eff= 13.5%

Page 11: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

11

Background study for B0→ψ' K π based upon BCS: Mbc

In order to study background, we use J/ψ inclusive MC (100 times data).

The background is expected to come from Bψ' K*(892) and B+ψ' K+π-π+.

Rest of the background is almost flat and can be taken care by 1st order polynomial while fitting

MJ/ψππ GeV/c2

Page 12: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

Background study for B0→ψ' K π based upon BCS:ΔE

MJ/ψππ GeV/c2

Page 13: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

K π mass distribution based upon BCS: Mbc

MKπ GeV/c2

B0→J/ψππ K*0 need to be handle with care in MKπ

Page 14: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

K π mass distribution based upon BCS:ΔE

MKπ GeV/c2

B0→J/ψππ K*0 need to be handle with care in MKπ

Page 15: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

15

Background study for X(3872) K π

MJ/ψππ GeV/c2

No serious background structure in X(3872) region.

Page 16: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

16

Background study for X(3872) K based upon ΔE

MJ/ψππ GeV/c2

No serious background structure in X(3872) region.

Page 17: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

K π mass distribution based upon BCS: Mbc

MKπ GeV/c2

B0→J/ψππ K*0 need to be handle with care in MKπ

Page 18: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

K π mass distribution based upon BCS:ΔE

MKπ GeV/c2

B0→J/ψππ K*0 need to be handle with care in MKπ

Page 19: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

19

Comparison with previous belle results

B → X(3872)K+π-

Efficiency (%)

BN999 8.9%

Results 13.5%

Page 20: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

20

Summaryi) Preliminary selection cuts and criteria has been done for B (J/ψππ) Kπ study.

ii) Signal generation has been done.

iii) Efficiency estimated by performing fit to MJ/ψππ.

iv) Background study is also done using J/ψ Inclusive MC.

v) Studying the background in ΔE and Mbc, revisiting BCS on the basis of background.

vi) No serious backgrounds but peaking background in MKπ needed to be handle with care.

vii) Strategy to extract signal yield will be developed.

Page 21: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

21

BACKUP

Page 22: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

BN 999

Page 23: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

BN 999

Page 24: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

BN 999

Page 25: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

25

Psikpi Mbc rec eff: 15.369%

25

Page 26: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

26

Psikstar Mbc rec eff : 14.87%

26

Page 27: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

27

Xkpi Mbc rec eff: 12.45%

27

Page 28: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

28

Xkstar Mbc rec eff: 13.6%

28

Page 29: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

Belle

6

29

KL

Page 30: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

The Belle Detector

SVD - Precise location of decay vertex• Electron/”hole” pairs generated

CDC - Particle tracks, momentum• Ionize gas, ions go to wires in cells, fit track

ACC - diff between K/π via Cerenkov• Designed for 1.2-3.5GeV(threshold)

TOF - PID• Scintillation, event time and pulse shape

30

Page 31: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

The Belle Detector

ECL - Electron/photon measurements• CsI crystal. Pair production, Bremsstrahlung

KLM -KL/Muon differentiation• Resistive plate chamber, iron for KL interaction

EFC - extension of ECL• BGO

31

Page 32: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π
Page 33: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

-- definitionsgood charged track:(this depends on evtcls default) Pt >= 0.1 GeV/c helix |dr|<2cm, |dz|<5cmgood ECL cluster: E(ECL cluster) > 0.1 GeVgood Gamma: E(ECL) > 0.1 GeVErec = Sum of Pcm(good charged track) in c.m.s. + SumSelection criteriaThe following list shows the curernt selection criteria for the tau skim. -- definitionsgood charged track:(this depends on evtcls default) Pt >= 0.1 GeV/c helix |dr|<2cm, |dz|<5cmgood ECL cluster: E(ECL cluster) > 0.1 GeVgood Gamma: E(ECL) > 0.1 GeVErec = Sum of Pcm(good charged track) in c.m.s. + Sum of Egamma in c.m.s.Ptmax : maximum Pt(good charged track)Etot = Erec + |Pmiss_CM|N_barrel: No. of track with 30< theta <130 degree (barrel region)E_ECL_trk = Sum of E(ECL) in c.m.s - Sum of Egamma in c.m.s.

33

Page 34: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

--- selection criteria1. 2<= No. of good track <=82. |charge sum|<=25. Ptmax > 0.5 GeV/c6m. Event vertex |r|<1cm,|z|<3cm7. for 2 track event 7-2m. Sum of E(ECL) < 11 GeV 7-3. 5 < theta(missing momentum) < 175 degree8. Erec > 3 GeV .or. Ptmax > 1.0 GeV/c9. for 2-4 charged track case 9-1m. Etot < 9 GeV .or. maximum opening angle < 175 degree .or. 2 < Sum of E(ECL) < 10 GeV 9-2. N_barrel >= 2 .or. E_ECL_trk < 5.3 GeV

34

Page 35: Study of B X(3872) K π - TIFRgmohanty/baw2012/anu1.pdf2 Motivation ⧫ X(3872) not a conventional charmonium state ⧫ Study of B X3872 K π (by K. Trabelsi, BN 999) B X3872 K π

35

Delte E & Mbc window

color & cabbibo

Model used

color in fitting

compete channel

j/psi MC based on mbcS