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Abstract
A golden age for heavy-quarkonium physics dawned a decade ago, initiated by the confluence of exciting advances in quantum chromodynamics (QCD) and an explosion of related experimental activity. The early years of this period were chronicled in the Quarkonium Working Group (QWG) CERN Yellow Report (YR) in 2004, which presented a comprehensive review of the status of the field at that time and provided specific recommendations for further progress. However, the broad spectrum of subsequent breakthroughs, surprises, and continuing puzzles could only be partially anticipated. Since the release of the YR, the BESII program concluded only to give birth to BESIII; the B-factories and CLEO-c flourished; quarkonium production and polarization measurements at HERA and the Tevatron matured; and heavy-ion collisions at RHIC have opened a window on the deconfinement regime. All these experiments leave legacies of quality, precision, and unsolved mysteries for quarkonium physics, and therefore beg for continuing investigations at BESIII, the LHC, RHIC, FAIR, the Super Flavor and/or Tau–Charm factories, JLab, the ILC, and beyond. The list of newly found conventional states expanded to include hc(1P), χc2(2P), \(B_{c}^{+}\), and ηb(1S). In addition, the unexpected and still-fascinating X(3872) has been joined by more than a dozen other charmonium- and bottomonium-like “XYZ” states that appear to lie outside the quark model. Many of these still need experimental confirmation. The plethora of new states unleashed a flood of theoretical investigations into new forms of matter such as quark–gluon hybrids, mesonic molecules, and tetraquarks. Measurements of the spectroscopy, decays, production, and in-medium behavior of \(c\bar{c}\), \(b\bar{b}\), and \(b\bar{c}\) bound states have been shown to validate some theoretical approaches to QCD and highlight lack of quantitative success for others. Lattice QCD has grown from a tool with computational possibilities to an industrial-strength effort now dependent more on insight and innovation than pure computational power. New effective field theories for the description of quarkonium in different regimes have been developed and brought to a high degree of sophistication, thus enabling precise and solid theoretical predictions. Many expected decays and transitions have either been measured with precision or for the first time, but the confusing patterns of decays, both above and below open-flavor thresholds, endure and have deepened. The intriguing details of quarkonium suppression in heavy-ion collisions that have emerged from RHIC have elevated the importance of separating hot- and cold-nuclear-matter effects in quark–gluon plasma studies. This review systematically addresses all these matters and concludes by prioritizing directions for ongoing and future efforts.
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1 Physik-Department, Technische Universität München, Garching, Germany
2 Budker Institute of Nuclear Physics, Novosibirsk, Russia; Novosibirsk State University, Novosibirsk, Russia
3 Cornell University, Ithaca, NY, USA
4 Physics Division, Lawrence Livermore National Laboratory, Livermore, CA, USA; Physics Department, University of California at Davis, Davis, CA, USA
5 High Energy Physics Division, Argonne National Laboratory, Argonne, IL, USA
6 Fermi National Accelerator Laboratory, Batavia, IL, USA
7 Physics Department, Florida State University, Tallahassee, FL, USA
8 Deutsches Elektronen-Synchrotron DESY, Hamburg, Germany
9 Indiana University, Bloomington, IN, USA
10 Physics Department, Brookhaven National Laboratory, Upton, NY, USA
11 Department of Physics and Astronomy, Wayne State University, Detroit, MI, USA
12 Laboratoire de l’Accélérateur Linéaire, IN2P3/CNRS and Université Paris-Sud 11, Centre Scientifique d’Orsay, Orsay Cedex, France
13 GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
14 INFN Sezione di Torino, Torino, Italy
15 Department of Physics, The Ohio State University, Columbus, OH, USA
16 Institut für Theoretische Physik, Universität Regensburg, Regensburg, Germany
17 INFN Sezione di Padova, Padova, Italy
18 Università di Ferrara and INFN Sezione di Ferrara, Ferrara, Italy
19 Institute of Nuclear Physics, Polish Academy of Sciences, Kraków, Poland
20 Università di Bari and INFN Sezione di Bari, Bari, Italy
21 Max Planck Institute for Physics, München, Germany
22 Department of Physics, Lancaster University, Lancaster, UK
23 CCAST (World Laboratory), Beijing, China; Institute of Theoretical Physics, Chinese Academy of Sciences, Beijing, China
24 Department of Physics, Peking University, Beijing, China
25 Thomas Jefferson National Accelerator Facility, Newport News, VA, USA
26 Clermont Université, Université Blaise Pascal, CNRS-IN2P3, LPC, Clermont-Ferrand, France
27 University of Cincinnati, Cincinnati, OH, USA
28 Laboratoire de Physique Théorique, Unité mixte de Recherche, CNRS, UMR 8627, Université de Paris-Sud, Orsay, France
29 LIP, Lisbon, Portugal
30 SLAC National Accelerator Laboratory, Stanford, CA, USA
31 Department of Physics, University of Alberta, Edmonton, Alberta, Canada
32 Institut für Kernphysik, Jülich Center for Hadron Physics, and Institute for Advanced Simulation, Forschungszentrum Jülich, Jülich, Germany
33 Department of Physics and Astronomy, University of Hawaii, Honolulu, HI, USA
34 Illinois Institute of Technology, Chicago, IL, USA
35 Lawrence Berkeley National Laboratory, Berkeley, CA, USA
36 IPNO, Université Paris-Sud 11, CNRS/IN2P3, Orsay, France; Centre de Physique Théorique, École Polytechnique, CNRS, Palaiseau, France
37 Budker Institute of Nuclear Physics, Novosibirsk, Russia
38 INFN Sezione di Milano, Milano, Italy
39 CERN, Geneva 23, Switzerland
40 Center for Cosmology, Particle Physics and Phenomenology, Université Catholique de Louvain, Louvain-la-Neuve, Belgium
41 Department of Math and Science, Pratt Institute, Brooklyn, NY, USA
42 Instituto de Física, Universidade de São Paulo, São Paulo, SP, Brazil
43 Department of Physics & Astronomy, Seoul National University, Seoul, Korea
44 Institute for Theoretical and Experimental Physics, Moscow, Russia
45 INFN Sezione di Roma, Roma, Italy
46 Laboratoire de l’Accélérateur Linéaire, IN2P3/CNRS and Université Paris-Sud 11, Centre Scientifique d’Orsay, Orsay Cedex, France; Department of Engineering Physics, Tsinghua University, Beijing, China
47 Physics Department, Brookhaven National Laboratory, Upton, NY, USA; C.N. Yang Institute for Theoretical Physics, Stony Brook University, Stony Brook, NY, USA
48 Institute of High Energy Physics, Chinese Academy of Sciences, Beijing, China
49 Instituto de Física Corpuscular (IFIC) and Departamento de Física Teórica, Centro Mixto Universitat de Valencia-CSIC, Burjassot, Valencia, Spain
50 Max Planck Institute for Physics, München, Germany; Excellence Cluster ‘Universe’, Technische Universität München, Garching, Germany
51 INFN Sezione di Milano, Milano, Italy; Dipartimento di Fisica, Università di Milano, Milano, Italy
52 Department of Physics, Tohoku University, Sendai, Japan
53 William I. Fine Theoretical Physics Institute, School of Physics and Astronomy, University of Minnesota, Minneapolis, MN, USA





