The observation of Z c (4025) Landiao Liu ( ) PKU ( ) UCAS ( - - PowerPoint PPT Presentation

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The observation of Z c (4025) Landiao Liu ( ) PKU ( ) UCAS ( - - PowerPoint PPT Presentation

The observation of Z c (4025) Landiao Liu ( ) PKU ( ) UCAS ( ) BESIII Collaboration Outline Introduction The observation of Zc(4025) +/- The observation of Zc(4025) 0 Summary 2 PART 1


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SLIDE 1

The observation of Zc(4025)

Landiao Liu (刘兰雕)

PKU (北京大学) UCAS (中国科学院大学) BESIII Collaboration

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SLIDE 2

Outline

  • Introduction
  • The observation of Zc(4025)+/-
  • The observation of Zc(4025)0
  • Summary

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SLIDE 3

PART 1

Introduction

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SLIDE 4
  • Quark Model
  • Exotic states predicted by QCD

𝑟 𝑟 𝑡 𝑣 𝑒 𝑣 𝑑 𝑑 𝑣 𝑣 𝑑 𝑑 𝑣 𝑣 𝑒 𝑡 𝑣 𝑒 𝑣 𝑡 𝑒 𝑡 𝑣 𝑒 𝑑 𝑑

Mesons

Color-anticolor pairs

Baryons

Red-blue-green triplets

Tetraquark

Tightly bound diquark&anti-diquark

Molecule

Loosely bound meson&anti-meson

Pentaquark

S=+1

Six-quark state

Tightly bound 6 quarks

Hybird

More than 2 quarks and gluon

Constitution of hadrons in QCD

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SLIDE 5
  • Below open charm threshold

Good agreement between discovery and theoretical prediction.

  • Above open charm threshold

Many expected states are not observed Many unexpected states are observed: XYZ states

Charmonium Spectroscopy

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SLIDE 6

Data samples for XYZ states at BESIII

  • Luminosity~5 fb-1
  • Large data samples around Ψ(4040), Y(4260), Y(4360), Ψ(4415) and Y(4660)

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SLIDE 7

Zc states at BESIII

  • Zc(3900)+/- in e+e- → π+ π- J/ Ψ

PRL 110,252001 (2013)

  • Zc(3900)0 in e+e- → π0 π0 J/ Ψ arXiv:1506.06018
  • Zc(3885)+/- in e+e- → π+ ( D

D∗)- PRL 112, 022001 (2014)

  • Zc(3885)0 in e+e- → π0 (D

D∗)0 Preliminary

  • Zc(4020)+/- in e+e- → π+ π- hc PRL 111.242001 (2013)
  • Zc(4020)0 in e+e- → π0 π0 hc PRL 113,212002 (2014)
  • Zc(4025)+/- in e+e- → π+ (D∗

D∗)- PRL 112,132001 (2013)

  • Zc(4025)0 in e+e- → π0 (D∗

D∗)0 arXiv:1507.02404

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SLIDE 8

e+e- →π Zc(3900)+/-/0 → π π J/ Ψ

  • Zc(3900)+/-, observed by BESIII, confirmed by Bell and

CLEO-c data.

  • Zc(3900)0, evidence with 3.7σ at CLEO-c, observed by

BESIII.

Zc(3900) Mass(MeV) Width(MeV) Zc(3900)+/- 3899.0±3.6±4.9 46 ±10±20 Zc(3900)0 3894.8±2.3±2.7 29.6±8.2±8.2

PRL 110,252001 (2013) arXiv:1506.06018 Zc(3900)+/- Zc(3900)0 Iso-spin triplet is established! 8

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SLIDE 9

e+e-→π Zc(3885)+/-/0 → π ( D D∗)

PRL 112.022001 (2014) preliminary

  • Zc(3885)+/-/0, observed by BESIII.
  • Have a mass and width close to Zc(3900).

Zc(3885) Mass(MeV) Width(MeV) Zc(3885)+/- 3883.9±1.5±4.2 24.8±3.3±1.0 Zc(3885)0 3885.7 −5.7

+4.3±8.4

35 −12

+11±15

Iso-spin triplet is established! Zc(3885)+/- Zc(3885)0 9

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e+e- →π Zc(4020)+/-/0 → π π hc

PRL 111,242001 (2013) PRL 113,212002 (2014)

  • Zc(4020)+/-/0, observed by BESIII.
  • A hint for Zc(3900)+/-/ → π+/- hc.
  • Zc(4020), near the D∗

D∗ threshold.

Zc(4020)+/- Zc(4020)0 Iso-spin triplet is established!

Zc(4020) Mass(MeV) Width(MeV) Zc(4020)+/- 4022.9±0.8±2.7 7.9±2.7±2.6 Zc(4020)0 4023.8±2.2±3.8 Fixed(=7.9)

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e+e-→π Zc(4025)+/-/0 → π (D∗ D∗)

PRL 111,242001 (2013) arXiv:1507.02404

Zc(4020) Mass(MeV) Width(MeV) Zc(4020)+/- 4026.3±2.6±3.7 24.8±5.6±7.7 Zc(4020)0 4025.5 −4.7

+2.0±3.1

23.0±6.0±1.0

  • Zc(4020)+/-/0, observed by BESIII.
  • The Zc(4020) and Zc(4025) are consistent within 1.5σ.
  • If they are the same state:

Γ(𝑎𝑑 4025 → D∗ D∗) Γ(𝑎𝑑(4020) → 𝜌ℎ𝑑) = 12 ± 5

Iso-spin triplet is established! 11

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SLIDE 12

Summary of Zc states at BESIII

e+e- → π+ π- J/ Ψ e+e- → π0 π0 J/ Ψ e+e- → π+ ( D D∗)- e+e- → π0 (D D∗)0 e+e- → π+ π- hc e+e- → π0 π0 hc e+e- → π+ ( D D∗)- e+e- → π0 (D D∗)0 Zc(3900)+/-? Zc(3900)0? Zc(4020)+/-? Zc(4020)0? 12

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SLIDE 13

PART 2

Zc(4025)+/-

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𝑬∗+ 𝑬∗𝟏 𝝆− 𝑬+ 𝑬𝟏 𝝆𝟏/𝜹 𝝆𝟏/𝜹

Topology

Particle will be detected Particle will not be detected Data @4260 𝝆− 𝑬+ Recoil mass of 𝝆− Single tag Select D*D*𝜌− process

Flow chart

One of the Pi0 should be detected 𝝆𝟏 Remove D*D* process 14

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Invariant mass of K- π+ π+

  • We reconstruct a D+ with only K- π+ π+.
  • The dots are data and histograms are MC.
  • The M(K- π+ π+) is required to be in (1.854,1.884)GeV/c2.

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D+ recoiling mass

  • The variable RM(D+)+M(D+)-m(D+) could improve the mass resolution by reducing the

correlation of RM(D+) and M(D+).

  • To remove the background e+e-->D(*) D(*), we require RM(D+)+M(D+)-m(D+) >2.3GeV/c2.

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SLIDE 17

Require an additional π0

  • M(γγ) lies in (0.12,0.145)GeV/c2.
  • π0 comes from D*+ or D*0.
  • Momentum of π0 in the RM(D+π-) lies in (0.03,0.05)GeV/c or M(D+π0)-

M(D+)+m(D+)-M(π0)+m(π0) lies in (2.008,2.013)GeV/c2. DATA MC 17

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SLIDE 18

D+ π- recoiling mass

DD* π process D* D* π process

  • The left peak corresponds to DD* π process while the right one

corresponds to D* D* π process

  • The green histogram is Wrong Sign. We use it to describe the

combinatorial backgrounds. 18

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Fit to data

  • Signal: efficiency-weighted S wave mass-dependent BW

convoluted with a detector resolution function.

  • Background: kernel-estimate of Wrong Sign Shape and its

magnitude is fixed to the number of the fitted background.

  • PHSP: The shape of the PHSP signal is taken from MC simulation

and its amplitude is taken as a free parameter. 19

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Systematic uncertainties

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D*D** process

  • Non-peaking type won’t contribute to the peak.
  • Type I: Much broader than the peak.
  • Type II: may affect the result, its amplitude need to be

decided through fit. 21

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SLIDE 22
  • Type I: add an additional component D*D**.
  • Fix its amplitude and obtain the shape from MC.
  • The resonance is still significance.
  • The change of results are considered as systematic

uncertainties.

  • Type II: add an additional component D*D**.
  • Float its amplitude and obtain the shape from

MC.

  • No sign of type II from the fit.

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PART 3

Zc(4025)0

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𝑬∗+ 𝑬∗− 𝝆𝟏

𝑬𝟏/𝑬+ 𝑬𝟏/𝑬− 𝝆+/𝟏/𝜹 𝝆−/𝟏/𝜹

𝝆𝟏/𝜹 𝑬𝟏

𝑬∗𝟏 𝝆𝟏 𝑬∗𝟏

𝝆𝟏/𝜹 𝑬𝟏

Topology

Particle will be detected Particle will not be detected Data @4230 /@4260 𝝆𝟏 𝑬𝟏/𝑬+ 𝑬𝟏/𝑬− Bachelor 𝝆𝟏 candidate Recoil mass of 𝝆𝟏 𝛿 veto(other showers) Double tag 𝜌0 is not from D* 𝜌0 is from D*D*𝜌0 process

Flow chart

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Double tag method

  • Tag a 𝐄 and a

𝐄

mode 0: D0 → K- π+ + c.c. mode 1: D0 → K- π+ π0 +c.c. mode 3: D0 → K- π+ π+ π- +c.c. mode 200: D+ → K- π+ π+ +c.c.

  • Choose the best combination with minimum R

R = χKF

2 (D) +χKF 2 (

D)

  • Why double tag?

Double tag will reduce the efficiency dramatically, but it will also remove lots of backgrounds. In our analysis, how to suppress the background is crucial. 25

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SLIDE 26

χKF

2

  • f K- π+ π+

We apply different cut for different mode: Mode 0, 3, 200: χKF

2 <15

Mode 1 : χKF

2 <20 26

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SLIDE 27

γ veto method

  • To reject backgrounds, each photon candidate originating from the

bachelor π0 is required not to form a π0 (M(γ γ))with any other photon in the event.

  • 𝛿 veto could rise the signal-to-background ratio dramatically.

Before veto After veto 𝛅 veto

Before After

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Select a good π0

(0.12,0.145)GeV/c2

  • After 𝛿 veto, the signal-to-background ratio

becomes good.

  • We require the Invariant mass of 𝜌0 lies in the

region (0.12,0.145)GeV/c2

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The invariant mass of D π0( D π0)

D*+ D*0

  • The deep color region corresponds to the D∗

peak

  • Since we should remove the π0 from D∗. We

require M(D π0) and M( D π0) are lager than 2.02GeV/c2. 29

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SLIDE 30

DD* π process D* D* π process

The recoil mass of D π0( D π0)

  • The left peak around 2GeV/c2 corresponds to the D* peak.
  • The right peak around 2.15GeV/c2 is produced by D* D*𝜌0 process.
  • The phase space of missing energy is limit, which includes a D* and a soft 𝜌 . Because of the soft 𝜌 , the peak
  • f RM(D π0) will shift up from D* to about 2.15GeV/c2. The resolution of the peak will be broadened slightly.

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SLIDE 31
  • Why oval cut?
  • val cut can removes more

background than quadrate cut.

  • Why oval @4230 is smaller than

@4260? the phase-space of missing energy @4230 is smaller than @4260, so the peak @4230 is sharper than @4260.

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Simultaneous fit

  • Signal: efficiency-weighted S wave mass-dependent BW

convoluted with a detector resolution function.

  • Background: kernel-estimate of Wrong Sign Shape and its

magnitude is fixed to the number of the fitted background.

  • PHSP: The shape of the PHSP signal is taken from MC simulation

and its amplitude is taken as a free parameter. 32

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SLIDE 33

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SLIDE 34

Mass(𝐍𝐟𝐖/𝐝𝟑) Width(𝐍𝐟𝐖/𝐝𝟑) 𝝉(𝒇+𝒇− → 𝒂𝒅(𝟓𝟏𝟑𝟔) 𝝆 → 𝑬∗ 𝑬∗𝝆 )(𝐪𝐜) @4.26GeV

𝒂𝒅(𝟓𝟏𝟑𝟔) 𝟏

𝟓𝟏𝟑𝟔. 𝟔−𝟓.𝟖

+𝟑,𝟏±𝟒. 𝟐

𝟑𝟒. 𝟏 ± 𝟕. 𝟏 ± 𝟐. 𝟏 𝟓𝟒. 𝟓 ± 𝟗. 𝟏 ± 𝟔. 𝟓

𝒂𝒅(𝟓𝟏𝟑𝟔) +

𝟓𝟏𝟑𝟕. 𝟒 ± 𝟑. 𝟕 ± 𝟒. 𝟖 𝟑𝟓. 𝟗 ± 𝟔. 𝟕 ± 𝟖. 𝟖 𝟓𝟑. 𝟑 ± 𝟑. 𝟗 ± 𝟓. 𝟕

Comparison between 𝐚𝐝(𝟓𝟏𝟑𝟔) 𝟏 and 𝐚𝐝(𝟓𝟏𝟑𝟔) +

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PART 3

Summary

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  • BESIII has observed serval Zc states. They should consist of at

least four quarks and considered as candidates of tetra-quark state.

  • Tetra-quarks or molecules?
  • e+e-->Zc ππ?
  • More Zc?

Thank you!

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