c c c c c c c c c c a Charmed baryon spectroscopy at Belle

Slides:



Advertisements
Similar presentations
Phi-Psi, Feb.-Mar., 2006, S.Uehara1 Experimental studies of charmonia in two-photon collisions at Belle S.Uehara (KEK) for the Belle Collaboration e +
Advertisements

Diquarks in heavy baryons Atsushi Hosaka (RCNP, Osaka U. ) 9/10-13, 2013Charmed baryons1 Practical questions of hadron physics How ground and excited states.
Excited Charm and K0sK0s Resonance Production at ZEUS V. Aushev For the ZEUS Collaboration XXXIX International Symposium on Multiparticle Dynamics ''Gold.
Properties and Decays of Heavy Flavor S-Wave Hadrons Rohit Dhir Department of Physics, Yonsei University, Seoul Dated:11 th June, 2012.
Likhoded A.K. IHEP, Protvino, Russia SuperB as a factory of Doubly Charmed Baryons?
Ruslan Chistov (ITEP, Moscow) Charm Baryon Spectroscopy at Belle Charm Charm Baryon Spectroscopy at Belle (1)Introduction to charmed baryons at.
Charm results overview1 Charm...the issues Lifetime Rare decays Mixing Semileptonic sector Hadronic decays (Dalitz plot) Leptonic decays Multi-body channels.
Spectroscopy of Heavy Quarkonia Holger Stöck University of Florida Representing the CLEO Collaboration 6 th International Conference on Hyperons, Charm.
Sep. 29, 2006 Henry Band - U. of Wisconsin 1 Hadronic Charm Decays From B Factories Henry Band University of Wisconsin 11th International Conference on.
DPF Victor Pavlunin on behalf of the CLEO Collaboration DPF-2006 Results from four CLEO Y (5S) analyses:  Exclusive B s and B Reconstruction at.
New Particles at BELLE Beauty 2005 Assisi Spectroscopy and new Particles F. Mandl There is an impressive list of new particles in the charm sector discovered.
Recent Results of Light Hadron Spectroscopy at BESIII Yutie LIANG (On behalf of the BESIII Collaboration) Justus-Liebig-Universität, Gieβen, Germany MESON.
1 The theoretical understanding of Y(4260) CONG-FENG QIAO Graduate School, Chinese Academy of Sciences SEPT 2006, DESY.
 c Physics at the Energy Threshold John Yelton U. of Florida CLEO experiment A review of what we know, and what we do not know, about the  c, with an.
Hadron Spectroscopy with high momentum beam line at J-PARC K. Ozawa (KEK) Contents Charmed baryon spectroscopy New experiment at J-PARC.
H. Koch, L.M.U. and T.U. Munich, Dec. 15, 2005 News with Charm  Introduction  Open Charm States  States with hidden Charm  Future: PANDA-Detector at.
New hadrons BaBar Maurizio Lo Vetere University of Genova & INFN Representing the Collaboration Particles and Nuclei International Conference.
P.Pakhlov ITEP, Moscow (for Belle collaboration) e+e- collision from  to  Novosibirsk, BINP, 2006.
Decay properties of D and D s mesons Bhavin Patel Department of Physics Sardar Patel University Vallabh Vidyanagar , Gujarat, INDIA.
Production rates of Strange and Charmed baryons at Belle 1  s = GeV Nuclear physics consortium.
Baryon Spectroscopy and Decays using the Belle Detector John Yelton University of Florida I review recent results on charmed baryon decay,
New Hadrons Newly observed D(2550), D(2610), and D(2760) as 2S and 1D charmed mesons “the same title”, Phys. Rev. D82 (2010) Observation of New.
D. Bettoni - The Panda experiment 1 Charmonium Spectroscopy The charmonium system has often been called the positronium of QCD. Non relativistic potential.
Hadron Physics at Belle
The study of pentaquark states in the unitary chiral approach
Maurizio Lo Vetere University of Genova & INFN
Maurizio Lo Vetere University of Genova & INFN
B States at the Tevatron
Spectroscopy Today BaBar’s Contributions
from Belle, BaBar and CLEO
Observation of the DsJ(2463)Dspo & Confirmation of the DsJ(2317)Dspo
Recent B physics results from BABAR and BELLE
Heavy quark spectroscopy and accurate prediction of b-baryon masses
Spectroscopy with Hyperon Beams
Charm spectroscopy 1 A. Drutskoy University of Cincinnati
Recent results on light hadron spectroscopy at BES
Y. Kato Nagoya University
The Renaissance in Hadron Spectroscopy
Possible Interpretations of DsJ(2632)
DsJ* ‘s & charmed strange baryons at Belle
PWA of J/pp0 and measurement of J/pp, pp'
Andrei Nomerotski (Oxford/Fermilab) ICHEP 2006, 29 July 2006
Section IX - Quark Model of Hadrons
Decoding the riddle of Y(4260) and Zc(3900) Qiang Zhao
Ye Li Graduate Student UW – Madison
Charm2010 4TH International Workshop on Charm Physics
charm baryon spectroscopy and decays at Belle
University of Minnesota on behalf of the CLEO Collaboration
Galina Pakhlova ITEP&Belle
The Quark-Diquark model description of double charm baryons
Charmed Baryon Spectroscopy and Decays using the Belle Detector
Λb and heavy states at Tevatron
e+e−→ open charm via ISR X(4160) in J/ recoil
Double charmonium production in e+e– annihilation
First discovery of Double Cabbibo-Suppressed decay: Lc  pK+p- + a
e+e−→ J/ D(*)D(*) & ψ(4160) → DD
Hadron spectroscopy results from Belle
CONVENTIONAL CHARMONIA
手征夸克模型的一些应用 钟显辉 湖南师范大学物理与信息科学学院.
Λb and heavy states at Tevatron
Recent Results on Charmonium from BaBar
Study of charmonium(-like) states at the Belle experiment
Hadron 2005 review Rio De Janeiro Aug >26 By Su Houng Lee
B. El-Bennich, A. Furman, R. Kamiński, L. Leśniak, B. Loiseau
Internal structure of f0(980) meson by fragmentation functions
Understanding DsJ*(2317) and DsJ(2460)
Exotic hadron physics at Belle II
New States Containing Charm at BABAR
Charmed Baryon Spectroscopy at BABAR
New Spectroscopy with Charm quarks at B factories.
Presentation transcript:

c c c c c c c c c c a Charmed baryon spectroscopy at Belle Y. Kato(KMI, Nagoya University) Phys. Rev. D 89, 052003 arXiv:1312.1026 c c Introduction Charmed strange baryons(Ξc) s s d a u c Physics of charmed baryons Ξc is a good probe to study u/d-s diquark system. This correlation can be studied only in the charm sector because in the strange sector, s quark is heavier than u/d quarks and weak u-d diquark correlation emerges. Charm quark is heavy (~1.5 GeV) compared with ..... Momentum of quarks inside the hadron (200 MeV) → Doubly charmed baryon is a good probe to study the potential between heavy quarks. Similar to the study of QQbar potential by charmonium spectroscopy. 2. Mass of u,d,s quarks (300-500 MeV) → Singly charmed baryon is a good probe to study the diquark correlation of light quarks. This is because spin-spin interaction is proportional to 1/m1m2. λmode s u ρ mode BaBar c c c c Belle Belle found Ξc(2980) and Ξc(3080) in the Λc+K-π+ final state. Later, BaBar studied the same final state. They required Λc+π+ mass to be Σc(*) and reported another two resonances, Ξc(3055) and Ξc(3123) Ξc(3080) Σc(2520) d u Σc(2455) c Ξc(2980) Ξc(2980) Ξc(3080) Ξc(3055)? Require Σc(2455) λ mode Ξc(3123)? Ξc(3080) q q ρmode Experimental situation M(Λc+K-π+) diquark Require Σc(2520) Re-analysis by Belle M(Λc+K-π+) ・All the ground states of single charmed baryon has discovered  mainly by e+e- collideer experiments like CLEO, BaBar, Belle. ・Many excited states has been also discovered. ・Almost no quantum numbers has been measured. ・No doubly charmed baryons including ground states. Ξc(2980)+ Ξc(3080)+ Ξc(3080)+ Ξc(3055) is confirmed in Σc(2455) K- while Ξc(3123) in Σc(2520) is not confirmed. U.L of the cross section is 0.34 fb ⇔ (1.6±0.6±0.2)fb by BaBar. Ξc(3055)+ spin=3/2 spin=1/2 charm Further study with ΛD final state ΛD0 ΛD+ M(ΛD0) D0 sideband M(ΛD0bar) M(ΛD+) D+ sideband M(ΛD-) Ξc(3055)+ Ξc(3055)0 We observe Ξc(3055)/(3080) in the ΛD final state. This is the first observation of the Ξc(3055)0. As discussed later, The relative branching fraction is sensitive to the excitation modes (ρ,λ) c c Ξc(3080)0 Search for doubly charmed baryons u Experimental situation ? The SELEX experiment in FNAL reported evidence of Ξcc+ in the Λc+K-π final state at 3520 MeV. However, this result was not supported by Belle, BaBar, Focus and LHCb. To discover the ground state is a big milestone. Discussion on the Ξc states Comparison of Λc+ and Ξc, Σc and Ξc’ New analysis by Belle Jp Λc+ (cud) Ξc (cus) ΔM(Mev/c2) Note 1/2+ Λc(2286)+ Ξc(2470) 181 ground state 1/2- Λc(2595)+ Ξc(2790) 194 Λ(1405) like 3/2- Λc(2625)+ Ξc(2815) 188 Λ(1520) like ?? Λc(2765)+? Ξc(2980)? 205 Isospin not determined 5/2+ Λc(2880)+ Ξc(3080)? 200 ・Use full statistics (980fb-1) of Belle data. =2 (4) times of previous Belle (BaBar) anslysis ・Study not only Λc+K-π+ final state but also Ξc0π+ decay mode (Belle studied Λc+K-π+ only but BaBar studied both) ・Add several sub decay of Λc+ (pK-π+, pKS0)and Ξc0 (Ξ-π+, ΛK-π+, pK-K-π+) → yield is increased by 20% for Λc+ and 3 times for Ξc0 spin0 di-quark Jp Σc Ξc’ ΔM(Mev/c2) Note 1/2+ Σc(2455) Ξc(2575) 120 ground state 3/2+ Σc(2520) Ξc(2645) 125 Σ(1385) like ?? Σc(2800) spin1 di-quark Ξc0π+ mode Λc+K-π+ mode Ξc0→Ξ-π+ Ξc0→pK-K-π+ ・Thee mass difference of Λc+ and Ξc is ~200 MeV, Σc and Ξc’ is ~120 MeV. Λc+ with 3055-200 = 2855 MeV, or Σc with 3055-120 = 2935 MeV ? Ξc(3055) is a pecial state by including strange quark?? Discussion from decay modes. Data Expectation of signal (assuming σ=500fb, Br=5%) Ξc0→ΛK-π+ Prediction from chiral quark model for relative branching fraction for Ξc(3055) arXiv:1205.2943 Lei-Hua Liu et al No significant signal! Close to the some of theoretical prediction. Possible to access in the BelleⅡ? Large branching fraction to ΛD is inconsistent Ξc(3055)/(3080) can decay into (heavy baryon+ light meson) and (light meson + heavy baryon) Σc Λ D K- UL of σ(e+e-→ΞccX)×Br(Ξcc+→Ξc0π+)×Br(Ξc+→Ξ-π+) σ(e+e-→ΞccX)×Br(Ξcc+→ΛcK-π+) c Naively thinking… λ mode→ (light baryon) + (heavy meson) ρ mode→ (heavy baryon) + (light meson) This study 4.1-25 fb Theory 3.5-10fb (assuming Br=5%) This study 0.076-0.35 fb Theory 0.175-0.5 fb (assuming Br=5%) λ mode s u Excitation of both λ and ρ mode? Further theoretical study is necessary. ρ mode