A Discovery of the tetraquark by the Belle Experiment

Similar documents
Exotic hadronic states XYZ

Searches for exotic mesons

Recent results for exo.c states from Belle

Kai Zhu on behalf of BESIII collaboration Institute of High Energy Physics, Beijing March, Moriond QCD 2015

Results on Charmonium-like States at BaBar

Heavy hadron spectroscopy at Belle. Kenkichi Miyabayashi (Nara Women s University) Hadrons and Hadron Interactions in QCD Mar.

Charmonium & charmoniumlike exotics

Hot Topic from Belle : Recent results on quarkonia

Chengping Shen: Beihang University, Beijing XVI International Conference on Hadron Spectroscopy (Hadron 2015) September, 2015, JLab, USA

Nouveaux Etats mésoniques découverts avec les usines

Heavy Quark Spectroscopy at LHCb

X states (X(3872),...)

Bottomonia & charmonia at B-factories

(for the BESIII Collaboration)

quarkonium XiaoLong Wang Key Laboratory of Nuclear Physics and Ion-beam Application (MOE) Institute of Modern Physics, Fudan University

Charmonium Radiative Transitions

Narrow States Near Thresholds: X(3872)

Recent XYZ results from Belle

Recent results and prospects of exotic hadrons at B-factory

University of Hawaii Colloquium Discovery of the Z c (3900)

Updates on X 3872 production at Belle. K.Trabelsi QWG6 Workshop Nara, Dec 2-5, 2008

Studies of charmonium production in e + e - annihilation and B decays at BaBar

Latest developments in the Spectroscopy of Heavy Hadrons

Vincent Poireau CNRS-IN2P3, LAPP Annecy, Université de Savoie, France On behalf of the BaBar collaboration

Nonstandard hadrons -- a few comments--

Charmonium Spectroscopy at BESIII

New types of sub-atomic particles

Recent Results from CLEO

Recent Results from the BESIII Experiment. Ryan Mitchell Indiana University Miami 2011 December 17, 2011

Puzzles in the Charmonium Sector of QCD

Meson Spectroscopy Methods, Measurements & Machines

Recent results on spectroscopy from

arxiv: v2 [hep-ex] 16 Nov 2007

Antimo Palano INFN and University of Bari, Italy On behalf of the LHCb Collaboration

Heavy flavor meson(-like) spectroscopy at Belle/Belle II. Kenkichi Miyabayashi Nara Women s at Tokai 2015 Aug.

Recent Results on J/ψ, ψ and ψ Decays from BESII

Zahra Haddadi, KVI-CART (University of Groningen) for the BESIII collaboration 1 Sep EUNPC 2015, Groningen

Studies of charmonium(-like) states at BESIII

CHARM MESON SPECTROSCOPY AT

MESON SPECTROSCOPY RESULTS

PoS(EPS-HEP 2009)057. Bottomonium Studies at BaBar. Veronique Ziegler. SLAC National Accelerator Laboratory

Recent Progress in Baryon Spectroscopy at BESIII

BaBar s Contributions. Veronique Ziegler Jefferson Lab

NEW PERSPECTIVES FOR STUDY OF CHARMONIUM AND EXOTICS ABOVE DD THRESHOLD. Barabanov M.Yu., Vodopyanov A.S.

Hadron Spectroscopy and Exotics Heavy Exotic Mesons Theory

VV process. Liu Zhiqing ( 劉智青 ) IHEP, Beijing. On behalf of Belle Collaboration.

Hadroproduction of Υ(nS) above the B B threshold and implications for Y b (10890)

Charmed Baryon spectroscopy at Belle 1. Y. Kato KMI topics. Mainly based on the paper recently accepted by PRD ( arxiv: )

arxiv: v2 [hep-ph] 2 Jan 2019

Charmonium and -like states from Belle

Tetraquark interpretation of e + e ϒπ + π Belle data and e + e b b BaBar data

Hadronic molecules with heavy quarks

LHCb Spectroscopy: Results and Plans

arxiv: v1 [hep-ex] 5 Nov 2015

CharmSpectroscopy from B factories

Some recent progresses in heavy hadron physics. Kazem Azizi. Oct 23-26, Second Iran & Turkey Joint Conference on LHC Physics

Charmonium(-like) and Bottomonium(-like) States Results from Belle and BaBar

Charmonium Physics. Zhengguo Zhao. University of Science and Technology of China (USTC) PIC2010 Karlsruhe, Zhengguo Zhao

Spectroscopy and Decay results from CDF

Search for exotic charmonium states

TETRAQUARKS AND PENTAQUARK(S)

ATLAS studies of spectroscopy and B-decays

e + e hadrons in ISR and Two-photon reactions with BELLE and BABAR

Study of Transitions and Decays of Bottomonia at Belle

Exotic hadrons at LHCb

CLEO Charmonium Results

Muoproduction of exotic charmonia at COMPASS

New bottomonium(-like) resonances spectroscopy and decays at Belle

Pentaquarks and Exotic Charm Spectroscopy at LHCb

Light Meson Decays at BESIII

Quarkonium Production and Decay

arxiv: v1 [hep-ex] 7 Aug 2014

Hadronic (ns) decays. VI International Workshop on Heavy Quarkonia, Elisabetta Prencipe On behalf of the BaBar collaboration

Charming Nuclear Physics

Popat Patel (McGill University) On behalf of the BaBar Collaboration The Lomonosov XIV Conference Moscow (2009/08/24)

Results on Charmonium(-like) and Bottomonium(-like) States from Belle and BaBar

Belle II and XYZ hadrons

Fulvio Piccinini. INFN, Sezione di Pavia

Prospects for Hadron Physics. Roberto Mussa INFN Torino

Hadron Spectroscopy with a variety of flavors

The BES-III experiment

Investigating different tetraquark structures for X(3872)

Exotic Quarkonium Spectroscopy and Production

Hadron Spectroscopy at LHCb

Hadron Spectroscopy at BESIII

Review of Light Hadron Spectra at BESIII

Pinning down the J PC values of the X(3872)

X(3872) and Its Production. 2nd workshop on the XYZ particles 11 月 21 日, 安徽黄山

Hadronic Charm Decays: Experimental Review

Quarkonium Physics at CMS

Coupled channel description for X(3872) and other XYZ mesons

Heavy Quark Baryons and Exotica

Update on X(3872) J PC determination

On the structure of X(3872) and Z(4430)

The newly discovered Ω c resonances and doubly charmed Ξ cc state. Kazem Azizi. Oct 4, School of Physics, IPM, Tehran- Iran

arxiv: v2 [hep-ph] 25 Nov 2014

XYZ par(cles at BESIII

Cusps, Resonances, and Exotic States. Eric Swanson

Hadronic molecules in effective field theory

Decays and productions of hadronic molecules

Transcription:

A Discovery of the tetraquark by the Belle Experiment Sookyung Choi (For the Belle Collabora5on) Gyeongsang Na5onal University JAGIELLONIAN Symposium, Krakow, Poland, June 9 2015 1

Outline X(3872) Charged Charmonium- like states : Z(4430), Z(4200), Charged Bo\omonium- like states : Z b s More charged charmonium- like states : Z c (3895),, more BESIII Z c s 2

Charmonium & Bo\omonium spectrum 3

cc assignments for the XYZ mesons? S Olsen, Front. Phys. 10, 101401 (2015) no unassigned levels for the 1 - - Y(4260) & Y(4360) Y(4360) Y(4260) X(4160) Z(4430) Z 2 (4250) Z(4200) the (5) charged Zs must have a minimal quark content of ccud Z(4050) Close to D*D* threshold X(3940) Y(3915) Z c (3900) X(3872) Close to D*D threshold the X(3940) & X(4160) as the η c (3S) & η c (4S) would imply huge hyperfine splittings for n=3&4 the Y(3915) mass and Γ(Y ωj/ψ) are too high for the χ c0 (2P) Neutral XYZ states Charged Z states 4

The list of XYZ states keeps growing (@2014) S Olsen, Front. Phys. 10, 101401 (2015) 5

Models for XYZ Mesons Tetra- quarks Hybrids u c c u c c u c π c u meson - molecules u c u c diquarkonium (diquark- dian5quarks) (π) c c (π) hadro - quarkonium Ispin triplet & singlet? neutral doublet charged doublet X(3872)YZ should have partner states: Three missing states in any pictures 6

The X(3872) B Kπ + π - J/ψ ψ π + π - J/ψ X(3872) π + π - J/ψ X(3872) aher 11 years (& >1000 cites, by 2014 Nov) 7

What do we know about the X(3872)? Belle BaBar BESIII CMS M X(3872) = 3871.69 ± 0.17 MeV m D 0 + m D* 0 = 3871.80 ± 0.17 MeV B.E. = 100 ± 210 kev Γ X(3872 < 1.2 MeV (90% CL) Y(4260) γx(3872)? 8

CDF PRL 98, 132002: J PC = 1 ++ or 2 - + J PC =1 ++ Belle PRD 84, 052004(R): J PC = 1 ++ or 2 - + 1 - - 1 ++, 2 - + 0 ++ LHCb PRL 110, 222001: J PC = 1 ++

Radia5ve decays of X(3872) : a probe of the nature of X(3872) X(3872) γ ψ, γ J/ψ C=+1 BaBar Belle LHCb From T. Skwarnicki (Moriond QCD 2015) 10

Strong decay X(3872) DD* 2- dim. Fit PRD81, 031103(2010) B K D 0 D *0 605 fb -1 6.4σ B + & D0 BD 0 π D 0 0 D *0 K M =3875.1 +0.7 0.5 414fb -1 B KD 0 D 0 π 0 ±0.5 MeV 347fb -1 D *0 D 0 γ D *0 D 0 π 0 BaBar PRD77, 011102(2008) Belle PRL97, 162002(2006) Both groups saw a high mass value & a Bf(DD*) 10x Bf(π + π - J/ψ) M = 3872.9 + 0.6 0.4 + 0.4 0.5 MeV Agrees with Mass from ππj/ψ mode Γ(BW) = 3.9 + 2.8 1.4 + 0.2 1.1 MeV B(B K X 3872 )xb(x 3872 D *0 D 0 ) = (0.80±0.20± 0.10)x10-4 11

Isospin of the X(3872) No X(3872) charged partner states in B Kπ + π 0 J/ψ (If M(X + ) > m D ++m D* 0 3877 MeV, Γ(X + ) may be wide) Belle PRD 84, 052004(R) & BaBar PRD 71, 031501 B 0 K - π + π 0 J/ψ m D ++m D* 0 B + K 0 π + π 0 J/ψ m D ++m D* 0 M(π + π 0 J/ψ) (GeV) M(π + π 0 J/ψ) (GeV) 12

Isospin mixing in the X(3872) X(3872) ρ J/ψ ω J/ψ Isospin viola5ng decay modes (each other) with similar BFs X(3872) D 0 D* 0 ~ 10 x BF(X J/ψππ ) Eric Braaten: S- wave DD* molecular components must exist D 0 D + D* - D* 0 X(3872) is mostly D 0 D* 0 > mixture of I=0 >& I=1> 13

CDF: ~85% of pp X(3872) is prompt D0: prompt pp X(3872)X pp ψ X D0 PRl 93, 162002 prompt X(3872) & ψ have similar produc5on characteris5cs (i.e. p T - & y - dependence, isola5on, etc.) D 0 B X(3872)+X c c ψ D* 0 14

hybrid model for the X(3872) e.g., Takizawa & Takeuchi PTEP 9, 093D01 D 0 D + D* - c c D* 0 X ωj/ψ decays X ρj/ψ decays produc5on 15

Charged Charmonium- like states : Z(4430), Z(4050), Z(4250), Z(4200) (new) and Z(3885).. 16

Belle : 660M BB The Z(4430) + Found by Belle in 2007 S- K Choi et al Belle: PRL 100 142001 R. Mizuk et al Belle: PRD 78 072004 5.2σ M(π + ψ ) Charged state cannot be Not seen by BaBar But both Data seems consistent Belle published two more results Latest one uses 4D amplitude analysis 17

Quantum numbers of the Z(4430) + Z(4430) + π + ψ in B Κ - π + ψ K Chilikin et al Belle: PRD 88 07402 (2013) Belle : 772 M BB 6.1σ Results from 4D fit M 2 (π + ψ ) 4485 MeV 18 1 + is favored over 0 - by 3.4 σ 18

Is Z(4430) + a resonance or resca\ering effect? Taken from T. Skwarnicki (Moriond QCD 2015) LHCb 19

The Z(4200) + New from Belle: 4- dim analysis of B K + π - J/ψ K Chilikin et al Belle: PRD 90 112009 (arxiv: 1408.6457 ) (2014) 20

New state Z(4200) + π - J/ψ 6.2 σ 13 +1 132 +1 1 + is favored over 0 - by 6.1σ and 2 - by 4.4 σ 21

Z(4430) + π - J/ψ B Kπ + J/ψ with Z(4430) 4.0σ no Z(4430) This may support the Z(4430) as an hadro- charmonium other than conven5onal tetraquark state M(Z c (4430))-M(Z c (3900)) = 589 ± 30 MeV M(ψ ) M(J/ψ) = 589 MeV Is Z(4430) a radial excita5on of the ground state of Z c (3900)? 22

Z(4050) + and Z(4250) + π + χ c1 in B 0 Κ - π + χ c1 PRD 78, 072004 (2008) > 5 σ 23

Charged Bo\omonium- like Z b states and neutral partner state: Z b (10610) +, Z b (10650) + and Z b (10610) 0 24

The Y(4260) σ(e + e - hadrons) found by BaBar in e + e - γ ISR π + π - J/ψ Confirmed by Cleo, Belle and BES BaBar PRD86, 051102 Γ(π + π - J/ψ) is large, 10~100 charmonium E cm (GeV) M(π + π - J/ψ) (GeV) Is there a b- quark version of Y(4260)? 25

bo\omonium bb mesons New Measurement of R b, R ϒ(nS)ππ Is there any anomaly in ϒ(4S,5S) π + π - ϒ (1S)? (Con5nuum subtrac5on and ISR correc5on applied) Lum ~1/20 th σ ~1/5 th Signal ~ 6 2S 3S 4S 5S Belle: PRL 100 112001 parent Γ(Y 4,5S ππϒ 1S ) ϒ(4S) ϒ(5S) 1.75 ± 0.35 kev 590 ± 110 kev Energy scan 26

ϒ(5S) π + π - ϒ (1,2,3S)? Belle PRL 108, 122001 (2012) 121.4 c - 1 π + π - M 2 (ϒπ ± ) Υ(3S)π + π - Υ(2S)π + π - M 2 (ϒπ ± ) π + π - Υ(1S)π + π - M 2 (ϒπ ± ) M 2 (π + π - ) 27

ϒ(5S) π + π - ϒ (1S)? Belle PRL 108, 122001 (2012) 121.4 c - 1 Υ(3S)π + π - π + π - M 2 (ϒπ ± ) M(ϒ(3S)π ± ) Υ(2S)π + π - π + π - Υ(1S)π + π - M(ϒ(2S)π ± ) M(ϒ(1S)π ± ) 28

ϒ(5S) π - Z + b1,2 Belle PRL 108, 122001 (2012) 121.4 c - 1 π + ϒ (1,2,3S) π + 10,610 MeV 10,660 MeV ϒ (3S) ϒ (2S) ϒ (1S) M(ϒ(nS)π + ) max 29

Bo\omonium spectrum ϒ(5S) π - Z b1,2 + Belle PRL 108, 122001 (2012) 121.4 c - 1 π + h b (1P, 2P) π + 10,610 MeV 10,660 MeV 30

Summary of parameter measurements m B +m B* 2m B* Belle PRL 108, 122001 B d b B* d b Z b (10610) M=10607.2±2.0 MeV Z b (10650) M=10652.2±1.5 MeV Γ=18.4±2.4 MeV Γ=11.5±2.2 MeV 31

Z b (10610) BB* & Z b (10650) B*B* ϒ(5S) π - (BB*) + ϒ(5S) π - (B*B*) + Z b (10610) ± Z b (10650) ± M(BB*) arxiv : 1209.6450 M(B*B*) Bf(Z b (10610) BB* Bf(Z b (10610) π + (bb) =6.2±0.7 Bf(Z b (10650) B*B* =2.8±0.4 Bf(Z b (10650) π + (bb) 32

Z b 0 search in ϒ(5S) π 0 π 0 ϒ (1,2S) Belle PRD 88 052016 (2013) 33

More Z c states 34

Discovery chain from Y(4260) to Z b(c) s by BaBar in e + e - γ ISR π + π - J/ψ Y(4260) discovered Is there a b- quark equivalent???? Yes, & it decays to Z b states Are there c- quark versions of Z b s? ϒ(5S) π + Ζ b - π + π - ϒ (1S) Yes, many Z c s!! 35

Z c (3895) by Belle e + e - (γ)y(4260) π - Z c (3895) + π + π - J/ψ PRL 110, 252002 (2013) arxiv:1304.0121 Y(4360) Y(4260) X(4160) X(3940) Z(4430) Z 2 (4250) π + Z(4050) Y(3915) Z c (3900) X(3872) BESIII data clearly establish J P =1 + From DD* π - Neutral XYZ states Charged Z states Mass = (3894.5 ± 6.6 ± 4.5) MeV Width = (63 ± 24 ± 26) MeV Fraction = (29.0 ± 8.9)% (stat. error only) Significance = 5.2 σ 36

Y(4260) π - Z c (3900) + π π + J/ψ BESIII: PRL 110, 252001 arxiv:1303.5949 Mass = (3899.0±3.6±4.9) MeV Width = (46±10±20) MeV Fraction = (21.5±3.3±7.5)% Significance > 8 σ 37

Z c states from BESIII 38

Summary of Z c states discovered in the BESIII experiment From Xu Xinping, C. Yuan (QWG2014) 39

Z(3900) 0 & Z(4020) 0 search at Belle From Anna Vinokurova at CHARM2015 arxiv : 1501:06351 JHEP.. M(η c π + π - ) (GeV) M(η c π + π - ) (GeV) 40

X(3872) and other 1 + XYZ states Molecules Level Diagram? (By S. Olsen Front. Phys. 10, 101401 (2015) The J P =1 + bo\omonium states? (See above ref.) 41

Belle discovered many XYZ states. Summary List of XYZ mesons keeps growing, however, their nature is s5ll in a mystery. Remains opportuni5es for LHCb and BelleII. 10 years aher the X(3872) s discovery, this is the most highly cited B- factory paper and BE = (m D* 0+ m D 0) - M X(3872) gets smaller, and now the BE= 0.1 +- 0.2MeV Models for the X(3872)YZ suggest the existence of addi5onal states Z(4430)+ from Belle is confirmed and J P is conclusively 1 +. Argand plot (LHCb) shows resonance behavior Charge and quantum numbers rule out conven5onal charmonium interpreta5on But s5ll non- resonant interpreta5on (resca\ering) possible. NEW charged state Z(4200) + is observed in B J/ψ π + K - decay. The quantum number is 1 +. Evidence of the Z(4430) + π + J/ψ is found. Z b (10610) +, Z b (10650) + and Z b (10610) 0 are the first candidate of ispin triplet in Belle. Many Z c states are recently discovered from BESIII (Belle) : including two sets of Isospin triplet states Z c (3900) and Z c (4020). 42

Back- up slides 43

M = 3872.0±0.6±0.5 MeV X(3872) ρj/ψ π + π - J/ψ X(3872) / γχ c1 M X(3872) m D 0+m D* 0 C=+ X(3872) 1 3 D 2 (ψ 2 ) 44

The Belle experiment TOF counter Peak luminosity recorded at KEKB: L=2.1 x 10 34 /cm 2 /sec with crab caviges 45

QCD hybrid? c c lightest 1 ++ hybrid ~4.4 GeV excited- state hybrids ground- state hybrids charmonium L Liu et al., JHEP 1207, 126 (2012) (Hadron Spectrum Collabora5on) 46

B 0 X(3872)K + π - PRD91, 051101 (R) (2015) B(B 0 X(K + π ) K*+NR ) B(X J/ψπ + π ) = (7.9±1.3±0.4) x 10 6 (B(B + X(K 0 π ) K*+NR ) B(X J/ψπ + π ) = (10.6±3.0±0.9) x 10 6 ) [both K*and (K+π ) NR ] 47

Results by Adding Z + (LHCb) K* vetoed 4- dim amplitude analysis B Kπ + ψ PRL 112, 222002 (2014) 48

Argand plot for Z c (4200) + Clearly shows Resonance-like change of the amplitude Much larger errors and impossible to Draw any conclusion yet. Unlike LHCb, Belle have two plots for two helicity amplitudes including higher waves. For S-wave, H 1 = H 0 49

Belle PRD 82, 091106R (2010) Energy scan to search for anomalous structure R ϒ(nS)ππ = Total 29.8 c - 1 R b = BaBar PRL 102, 012001 (2009) 10.865 ± 0.008 GeV Recall Y(4260) with anomalous Γ(J/ψ π + π - ) Is there a ϒ b equivalent close to ϒ(5S) 50

B- B* & B*- B* molecules?? B Z b (10610) ± Z b (10650) ± b B* b b B- B* molecule B* b B* B*- B* molecule M Zb (10610) (M B +M B* ) = + 2.7 ± 2.1 MeV M Zb (10650) 2M B* = + 2.0 ± 1.8 MeV Slightly unbound threshold resonances?? Belle: M=10607.2±2.0 MeV Γ=18.4±2.4 MeV M=10652.2±1.5 MeV Γ=11.5±2.2 MeV PDG: M B + M B* = 10604.5±0.6 MeV M B* + M B* = 10650.2 ± 1.0 MeV 51

BESIII collected 5 /ƒ above 4GeV for XYZ study BESIII Y(4260) γx(3872) 52

CLEOc data at 4.17 GeV: 1304.3036 M = 3885±5±1 MeV Γ = 34±12±4 MeV 81 ± 20 events 6.1σ 53

Z c (3900) 0? ( a neutral isospin partner state) Z c (3900) 0 First hint from 54

Search for Z c (3900) 0 Z c (3900) 0 This establishes the Isospin triplet of Z c (3900) 55