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A New Hadron Spectroscopy
Front. Phys. 10, 101401 (2015) DOI 10.1007/s11467-014-0449-6 REVIEW ARTICLE A new hadron spectroscopy Stephen Lars Olsen Center for Underground Physics, Institute of Basic Science, Daejeon 305-811, Korea E-mail: [email protected] Received August 13, 2014; accepted September 16, 2014 QCD-motivated models for hadrons predict an assortment of “exotic” hadrons that have structures that are more complex than the quark-antiquark mesons and three-quark baryons of the original quark-parton model. These include pentaquark baryons, the six-quark H-dibaryon, and tetraquark, hybrid and glueball mesons. Despite extensive experimental searches, no unambiguous candidates for any of these exotic configurations have been identified. On the other hand, a number of meson states, one that seems to be a proton-antiproton bound state, and others that contain either charmed- anticharmed quark pairs or bottom-antibottom quark pairs, have been recently discovered that neither fit into the quark-antiquark meson picture nor match the expected properties of the QCD- inspired exotics. Here I briefly review results from a recent search for the H-dibaryon, and discuss some properties of the newly discovered states –the proton-antiproton state and the so-called XYZ mesons– and compare them with expectations for conventional quark-antiquark mesons and the predicted QCD-exotic states. Keywords quarks, charmonium, pentaquarks, di-baryons, baryonium, tetraquarks PACS numb ers 14.40.Gx, 12.39.Mk, 13.20.He Contents gluons are related to mesons and baryons by the long- distance regime of Quantum Chromodynamics (QCD), 1 Introduction 1 which remains the least understood aspect of the the- 2 Pentaquarks and H-dibaryons 2 ory. -
Hadron and Quarkmonium Exotica
November 8, 2018 7:26 WSPC/INSTRUCTION FILE schoi-pic2013 International Journal of Modern Physics: Conference Series c World Scientific Publishing Company HADRON AND QUARKMONIUM EXOTICA Sookyung Choi Department of Physics, Gyeongsang National University Jinju daero 501, Jinju, 660-773, Republic of KOREA [email protected] Received Day November 2013 Revised Day Month Year A number of charmonium-(bottmonium-)like states have been observed in B-factory experiments. Recently the BESIII experiment has joined this search with a unique data sample collected at the different center of mass energies ranging from 3.9 GeV to 4.42 GeV in which they found new charmonium-like states with non-zero electric charge. We review the status of experimental searchs for quarkomonium-like states and also other types of non-qq¯ meson or non-qqq baryons that are predicted by QCD-motivated models. We mainly focus on results from the B-factories and BESIII. Keywords: PACS numbers: 1. Introduction Mesons and baryons are formed from color-singlet combinations of quarks. All non- qq¯ mesons and non-qqq baryons predicted by QCD-motivated models are expected arXiv:1403.1832v1 [hep-ex] 7 Mar 2014 to be in color-singlet multi-quark combinations. Color-singlet multiquark states can be formed from colored diquarks and dian- tiquarks: a pentaquark is predicted to contain two diquarks and one antiquark, the H-dibaryon contains three diquarks, and tetraquark mesons contain a diquark and diantiquark. Multiquark states can also be formed by molecules of two (or more) color-singlet qq¯ mesons and/or qqq baryons that are bound together by the exchange of virtual π σ, ω, etc. -
Ph.D. AC1.H3 5032 R.Pdf
UNIVERSITY OFf-IAWAI'1 LIBRARY AN ANALYSIS OF THE K+1l"+1l"- FINAL STATE IN A DISSERTATION SUBMITTED TO THE GRADUATE DMSION OF THE UNIVERSITY OF HAWAI'I IN PARTIAL FULFILLMENT OF THE REQUIREMENTS FOR THE DEGREE OF DOCTOR OF PHILOSOPHY IN PHYSICS MAY 2008 By Hulya Guler Dissertation Committee: Stephen L. Olsen, Chairperson Thomas E. Browder Sandip Pakvasa John M. J. Madey Kathleen C. Ruttenberg We certify that we have read this dissertation and that, in our opinion, it is satisfactory in scope and quality 118 a dissertation for the degree of Doctor of Philosophy in Physics. DISSERTATION COMMI'ITEE ii © 2008, HuIya GuIer iii Anneanneciifime. Hatice Giir 1919-2007 iv Acknowledgements I thank Stephen Olsen, Thomas Browder, Sandip PakvaBa, John Madey, and Kathleen Ruttenberg for serving on my committee. I am especially indebted to my advisor Stephen Olsen for his support and for trusting me enough to let me work inde pendently. I also thank ThomaB Browder, Sookyung Choi, ThomaB Dombeck, Fang Fang, Alexei GarmaBh, Li Jin, Michael Jones, Kay Kinoshita, Alexander Kuzmin, Jimmy Macnaughton, Daniel Marlow, Kenkichi MiyabayaBhi, Shohei Nishida, Sandip PakvaBa, Michael Peters, Yoshihide Sakai, Karim Trabelsi, Gary Varner, and Hitoshi Yamamoto for helpful discussions. I thank my mother, Bema Giir, for the sacrifices she haB made to enable me to pursue my interest in physics. I thank Jamal Rorie for being the ideal officemate and for his patience and un derstanding aB I worked on this thesis. I am grateful to my friends who have supported and encouraged me; in particu lar: Gene Altman, Javier Ferrandis, Tamar Friedmann, Jeanne Hogan, Abidin Kaya, Elena Martin, Miifit Tecimer, and Melek Yal!tmt~. -
BABAR Collaboration
SelectedSelected NewNew ResultsResults onon HeavyHeavy QuarksQuarks fromfrom XXXVI SLAC Summer Institute “Cosmic Accelerators” Tuesday, August 5, 2008 Alexandre (Sasha) Telnov Princeton University on behalf of the BABAR Collaboration SLAC, Mail Stop 35 2575 Sand Hill Road Menlo Park, CA 94025 [email protected] TheThe PEPPEP--IIII AcceleratorAccelerator ComplexComplex Reusing the SLAC linear accelerator (1966-present) and the PEP tunnel 467 ± 5 million BB pairs produced Nominal center-of-mass energy: 10.580 GeV — the ϒ(4S) bb resonance Beam energies: 9.0 GeV e−, 3.1 GeV e+ s e Number of bunches: up to 1722 il m .0 2 Peak luminosity: 12.1 x 1033 cm–1s–2 (original design: 3 x 1033 cm–1s–2) Best 24 hours: 911 pb–1 delivered (original design: 135 pb-1/day) − + 2200 m Peak beam currents: 2.05 A e , 3.03 A e circumference Luminous region (σX × σY): 125 µm × 4 µm SSI 2008: New Results on Heavy Quarks from BABAR Alexandre Telnov (Princeton), August 5, 2008 2 TheThe BBAABBARAR DetectorDetector Built by a collaboration of ~80 universities and labs from 11 countries SSI 2008: New Results on Heavy Quarks from BABAR Alexandre Telnov (Princeton), August 5, 2008 3 TheThe BBAABBARAR Detector:Detector: OutlineOutline Highlights to follow: SVT and DIRC Photon and KL detection, Electro-Magnetic Calorimeter Instrumented Flux Return electron identification 6580 crystals, Cesium Iodide doped with Thallium 12-18 layers of absorber (iron, brass) and muon detectors (RPC, LST) Detector of Internally Reflected Muon and KL identification Cherenkov Radiation Particle -
A Discovery of the Tetraquark by the Belle Experiment
A Discovery of the tetraquark by the Belle Experiment Sookyung Choi (For the Belle Collaboraon) Gyeongsang Naonal University JAGIELLONIAN Symposium, Krakow, Poland, June 9 2015 1 Outline • X(3872) • Charged Charmonium-like states : Z(4430), Z(4200), … • Charged Boomonium-like states : Zb’s • More charged charmonium-like states : Zc (3895), … , more BESIII Zc’s 2 Charmonium & Boomonium spectrum _ 3 cc assignments for the XYZ mesons? _ S Olsen, Front. Phys. 10, 101401 (2015) Z(4430) no unassigned levels for - - Y(4360) the (5) charged Zs the 1 Y(4260) & Y(4360) _ must have a minimal _ Y(4260) Z2(4250) quark content of ccud X(4160) Z(4200) Z(4050) Close to D*D* threshold X(3940) Y(3915) Zc(3900) X(3872) Close to D*D threshold the X(3940) & X(4160) as the Y(3915) mass and the ηc(3S) & ηc(4S) would Γ(Y ωJ/ψ) are too imply huge hyperfine high for the χc0(2P) splittings for n=3&4 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 _ u c Hybrids _ u _ c _ c c (π) _ c _ c _ u _ π u _ c _ u c _ u c (π) c meson - molecules diquarkonium hadro - quarkonium (diquark-dian5quarks) Ispin triplet neutral doublet & singlet ? charged doublet X(3872)YZ should have partner states: Three missing states in any pictures 6 The X(3872) BKπ+π-J/ψ ψ’π+π-J/ψ X(3872)π+π-J/ψ X(3872) aer 11 years (& >1000 cites, by 2014 Nov) 7 What do we know about the X(3872)? Belle BaBar BESIII CMS Y(4260) γX(3872)? MX(3872) = 3871.69 ± 0.17 MeV mD0 + mD*0 = 3871.80 ± 0.17 MeV “B.E.” = 100 ± 210 keV 8 ΓX(3872< 1.2 MeV (90% CL) JPC=1++ Belle PRD 84, 052004(R): JPC = 1++ or 2-+ CDF PRL 98, 132002: JPC = 1++ or 2-+ 1-- 1++, 2-+ 0++ LHCb PRL 110, 222001: JPC = 1++ Radiave decays of X(3872) : a probe of the nature of X(3872) C=+1 X(3872) γ ψ’, γ J/ψ BaBar Belle LHCb From T. -
December 6, 2013 23:51 WSPC/INSTRUCTION FILE Schoi-Pic2013-F
December 6, 2013 23:51 WSPC/INSTRUCTION FILE schoi-pic2013-f International Journal of Modern Physics: Conference Series c World Scientific Publishing Company HADRON AND QUARKMONIUM EXOTICA Sookyung Choi Department of Physics, Gyeongsang National University Jinju daero 501, Jinju, 660-773, Republic of KOREA [email protected] Received Day November 2013 Revised Day Month Year A number of charmonium-(bottmonium-)like states have been observed in B-factory experiments. Recently the BESIII experiment has joined this search with a unique data sample collected at the different center of mass energies ranging from 3.9 GeV to 4.42 GeV in which they found new charmonium-like states with non-zero electric charge. We review the status of experimental searchs for quarkomonium-like states and also other types of non-qq¯ meson or non-qqq baryons that are predicted by QCD-motivated models. We mainly focus on results from the B-factories and BESIII. Keywords: PACS numbers: 1. Introduction Mesons and baryons are formed from color-singlet combinations of quarks. All non- qq¯ mesons and non-qqq baryons predicted by QCD-motivated models are expected to be in color-singlet multi-quark combinations. Color-singlet multiquark states can be formed from colored diquarks and dian- tiquarks: a pentaquark is predicted to contain two diquarks and one antiquark, the H-dibaryon contains three diquarks, and tetraquark mesons contain a diquark and diantiquark. Multiquark states can also be formed by molecules of two (or more) color-singlet qq¯ mesons and/or qqq baryons that are bound together by the exchange of virtual π σ, ω, etc.