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
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
Landiao Liu (刘兰雕)
PKU (北京大学) UCAS (中国科学院大学) BESIII Collaboration
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Introduction
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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
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Good agreement between discovery and theoretical prediction.
Many expected states are not observed Many unexpected states are observed: XYZ states
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PRL 110,252001 (2013)
D∗)- PRL 112, 022001 (2014)
D∗)0 Preliminary
D∗)- PRL 112,132001 (2013)
D∗)0 arXiv:1507.02404
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CLEO-c data.
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
PRL 112.022001 (2014) preliminary
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
PRL 111,242001 (2013) PRL 113,212002 (2014)
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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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
Γ(𝑎𝑑 4025 → D∗ D∗) Γ(𝑎𝑑(4020) → 𝜌ℎ𝑑) = 12 ± 5
Iso-spin triplet is established! 11
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
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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correlation of RM(D+) and M(D+).
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M(D+)+m(D+)-M(π0)+m(π0) lies in (2.008,2.013)GeV/c2. DATA MC 17
DD* π process D* D* π process
corresponds to D* D* π process
combinatorial backgrounds. 18
convoluted with a detector resolution function.
magnitude is fixed to the number of the fitted background.
and its amplitude is taken as a free parameter. 19
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decided through fit. 21
uncertainties.
MC.
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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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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.
R = χKF
2 (D) +χKF 2 (
D)
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
2
We apply different cut for different mode: Mode 0, 3, 200: χKF
2 <15
Mode 1 : χKF
2 <20 26
bachelor π0 is required not to form a π0 (M(γ γ))with any other photon in the event.
Before veto After veto 𝛅 veto
Before After
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(0.12,0.145)GeV/c2
becomes good.
region (0.12,0.145)GeV/c2
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D*+ D*0
peak
require M(D π0) and M( D π0) are lager than 2.02GeV/c2. 29
DD* π process D* D* π process
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background than quadrate cut.
@4260? the phase-space of missing energy @4230 is smaller than @4260, so the peak @4230 is sharper than @4260.
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convoluted with a detector resolution function.
magnitude is fixed to the number of the fitted background.
and its amplitude is taken as a free parameter. 32
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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
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Summary
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least four quarks and considered as candidates of tetra-quark state.
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