Exotic Hadronic States
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LHC Explore Pentaquark
LHC Explore Pentaquark Scientists at the Large Hadron Collider have announced the discovery of a new particle called the pentaquark. [9] CERN scientists just completed one of the most exciting upgrades on the Large Hadron Collider—the Di-Jet Calorimeter (DCal). [8] As physicists were testing the repairs of LHC by zipping a few spare protons around the 17 mile loop, the CMS detector picked up something unusual. The team feverishly pored over the data, and ultimately came to an unlikely conclusion—in their tests, they had accidentally created a rainbow universe. [7] The universe may have existed forever, according to a new model that applies quantum correction terms to complement Einstein's theory of general relativity. The model may also account for dark matter and dark energy, resolving multiple problems at once. [6] This paper explains the Accelerating Universe, the Special and General Relativity from the observed effects of the accelerating electrons, causing naturally the experienced changes of the electric field potential along the moving electric charges. The accelerating electrons explain not only the Maxwell Equations and the Special Relativity, but the Heisenberg Uncertainty Relation, the wave particle duality and the electron’s spin also, building the bridge between the Classical and Relativistic Quantum Theories. The Big Bang caused acceleration created the radial currents of the matter and since the matter composed of negative and positive charges, these currents are creating magnetic field and attracting forces between the parallel moving electric currents. This is the gravitational force experienced by the matter, and also the mass is result of the electromagnetic forces between the charged particles. -
Pentaquark Search Shows How Science Moves Forward
Although initial results were encouraging, physicists searching for an exotic five-quark particle now think it probably doesn’t exist. The debate over the pentaquark search shows how science moves forward. The rise and fall of the PE NTAQUAR K by Kandice Carter, Jefferson Lab 16 Three years ago, research teams around the stars are made. Yet he and his peers had no world announced they had found data hinting at means to verify its existence. the existence of an exotic particle containing Luminaries of 16th-19th century physics, five quarks, more than ever observed in any other including Newton, Fresnel, Stokes, and Maxwell, quark-composite particle. More than two dozen debated at length the properties of their physi- experiments have since taken aim at the particle, cal version of the philosophical concept, which dubbed the pentaquark, and its possible partners, they called ether. in the quest to turn a hint into a discovery. It’s a The ether was a way to explain how light scenario that often plays out in science: an early could travel through empty space. In 1881, theory or observation points to a potentially Albert A. Michelson began to explore the ether important discovery, and experimenters race to concept with experimental tools. But his first corroborate or to refute the idea. experiments, which seemed to rule out the “Research is the process of going up alleys to existence of the ether, were later realized to be see if they are blind,” said Marston Bates, a zool- inconclusive. ogist whose research on mosquitoes led to Six years later, Michelson paired up with an understanding of how yellow fever is spread. -
Introduction to Subatomic- Particle Spectrometers∗
IIT-CAPP-15/2 Introduction to Subatomic- Particle Spectrometers∗ Daniel M. Kaplan Illinois Institute of Technology Chicago, IL 60616 Charles E. Lane Drexel University Philadelphia, PA 19104 Kenneth S. Nelsony University of Virginia Charlottesville, VA 22901 Abstract An introductory review, suitable for the beginning student of high-energy physics or professionals from other fields who may desire familiarity with subatomic-particle detection techniques. Subatomic-particle fundamentals and the basics of particle in- teractions with matter are summarized, after which we review particle detectors. We conclude with three examples that illustrate the variety of subatomic-particle spectrom- eters and exemplify the combined use of several detection techniques to characterize interaction events more-or-less completely. arXiv:physics/9805026v3 [physics.ins-det] 17 Jul 2015 ∗To appear in the Wiley Encyclopedia of Electrical and Electronics Engineering. yNow at Johns Hopkins University Applied Physics Laboratory, Laurel, MD 20723. 1 Contents 1 Introduction 5 2 Overview of Subatomic Particles 5 2.1 Leptons, Hadrons, Gauge and Higgs Bosons . 5 2.2 Neutrinos . 6 2.3 Quarks . 8 3 Overview of Particle Detection 9 3.1 Position Measurement: Hodoscopes and Telescopes . 9 3.2 Momentum and Energy Measurement . 9 3.2.1 Magnetic Spectrometry . 9 3.2.2 Calorimeters . 10 3.3 Particle Identification . 10 3.3.1 Calorimetric Electron (and Photon) Identification . 10 3.3.2 Muon Identification . 11 3.3.3 Time of Flight and Ionization . 11 3.3.4 Cherenkov Detectors . 11 3.3.5 Transition-Radiation Detectors . 12 3.4 Neutrino Detection . 12 3.4.1 Reactor Neutrinos . 12 3.4.2 Detection of High Energy Neutrinos . -
Photoproduction of Exotic Hadrons Exotic Mesons Photoproduction + Photoproduction of LHCB Pentaquarks
Introduction The MesonEx experiment The GlueX experiment Hidden-charm pentaquark search Conclusions Photoproduction of exotic hadrons Exotic mesons photoproduction + photoproduction of LHCB pentaquarks Andrea Celentano INFN-Genova Introduction The MesonEx experiment The GlueX experiment Hidden-charm pentaquark search Conclusions Introduction 1 Introduction 2 The MesonEx experiment 3 The GlueX experiment 4 Hidden-charm pentaquark search 5 Conclusions 2 / 24 Introduction The MesonEx experiment The GlueX experiment Hidden-charm pentaquark search Conclusions Exotic mesons QCD does not prohibit the existence of unconventional meson states such as hybrids (qqg), tetraquarks (qqqq), and glueballs. Exotic quantum numbers: J PC 6= qq The discovery of states with manifest gluonic component, behind the CQM, would be the opportunity to directly “look” inside hadron dynamics. Exotic quantum numbers would provide an unambiguous evidence of these states. Lattice QCD calculations1provided a first hint on the spectrum and mass range of exotics. Mass range: 1.4 GeV - 3.0 GeV CQM mesons Exotics Lightest exotic is a 1-+ state. Negative parity Positive parity 1 J. J. Dudek et al, Phys. Rev. D82, 034508 (2010) 3 / 24 Introduction The MesonEx experiment The GlueX experiment Hidden-charm pentaquark search Conclusions Exotic mesons photoproduction Traditionally, meson spectroscopy was studied trough different experimental techinques: peripheral hadron production, NN annihiliation, ... Photo-production measurements were limited by the lack of high-intensity, high-energy, high-quality photon beams. Today, this limitation is no longer present. Advantages: • Photon spin: exotic quantum numbers are more likely produced by S = 1 probe • Linear polarization: acts like a filter to disentangle the production mechanisms and suppress backgrounds • Production rate: for exotics is expected to be comparable as for regular meson 4 / 24 Introduction The MesonEx experiment The GlueX experiment Hidden-charm pentaquark search Conclusions Results from past experiments See P. -
Review of Lepton Universality Tests in B Decays
January 4, 2019 Review of Lepton Universality tests in B decays Simone Bifani∗, S´ebastienDescotes-Genony, Antonio Romero Vidalz, Marie-H´el`ene Schunex Abstract Several measurements of tree- and loop-level b-hadron decays performed in the recent years hint at a possible violation of Lepton Universality. This article presents an experimental and theoretical overview of the current status of the field. arXiv:1809.06229v2 [hep-ex] 3 Jan 2019 Published in Journal of Physics G: Nuclear and Particle Physics, Volume 46, Number 2 ∗University of Birmingham, School of Physics and Astronomy Edgbaston, Birmingham B15 2TT, United Kingdom yLaboratoire de Physique Th´eorique(UMR 8627), CNRS, Universit´eParis-Sud, Universit´eParis-Saclay, 91405 Orsay, France zInstituto Galego de F´ısicade Altas Enerx´ıas(IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain xLaboratoire de l'Acc´el´erateurLin´eaire,CNRS/IN2P3, Universit´eParis-Sud, Universit´eParis-Saclay, 91440 Orsay, France Contents 1 Introduction 1 2 Lepton Universality in the Standard Model 2 3 Overview of Lepton Universality tests beyond the B sector 3 3.1 Electroweak sector . .4 3.2 Decays of pseudoscalar mesons . .5 3.3 Purely leptonic decays . .7 3.4 Quarkonia decays . .7 3.5 Summary . .7 4 Theoretical treatment of b-quark decays probing Lepton Universality 8 4.1 Effective Hamiltonian . .8 4.2 Hadronic quantities . 10 4.3 Lepton Universality observables . 13 5 Experiments at the B-factories and at the Large Hadron Collider 13 5.1 B-factories . 13 5.2 Large Hadron Collider . 16 5.3 Complementarity between the B-factories and the LHC . -
Snowmass 2021 Letter of Interest: Hadron Spectroscopy at Belle II
Snowmass 2021 Letter of Interest: Hadron Spectroscopy at Belle II on behalf of the U.S. Belle II Collaboration D. M. Asner1, Sw. Banerjee2, J. V. Bennett3, G. Bonvicini4, R. A. Briere5, T. E. Browder6, D. N. Brown2, C. Chen7, D. Cinabro4, J. Cochran7, L. M. Cremaldi3, A. Di Canto1, K. Flood6, B. G. Fulsom8, R. Godang9, W. W. Jacobs10, D. E. Jaffe1, K. Kinoshita11, R. Kroeger3, R. Kulasiri12, P. J. Laycock1, K. A. Nishimura6, T. K. Pedlar13, L. E. Piilonen14, S. Prell7, C. Rosenfeld15, D. A. Sanders3, V. Savinov16, A. J. Schwartz11, J. Strube8, D. J. Summers3, S. E. Vahsen6, G. S. Varner6, A. Vossen17, L. Wood8, and J. Yelton18 1Brookhaven National Laboratory, Upton, New York 11973 2University of Louisville, Louisville, Kentucky 40292 3University of Mississippi, University, Mississippi 38677 4Wayne State University, Detroit, Michigan 48202 5Carnegie Mellon University, Pittsburgh, Pennsylvania 15213 6University of Hawaii, Honolulu, Hawaii 96822 7Iowa State University, Ames, Iowa 50011 8Pacific Northwest National Laboratory, Richland, Washington 99352 9University of South Alabama, Mobile, Alabama 36688 10Indiana University, Bloomington, Indiana 47408 11University of Cincinnati, Cincinnati, Ohio 45221 12Kennesaw State University, Kennesaw, Georgia 30144 13Luther College, Decorah, Iowa 52101 14Virginia Polytechnic Institute and State University, Blacksburg, Virginia 24061 15University of South Carolina, Columbia, South Carolina 29208 16University of Pittsburgh, Pittsburgh, Pennsylvania 15260 17Duke University, Durham, North Carolina 27708 18University of Florida, Gainesville, Florida 32611 Corresponding Author: B. G. Fulsom (Pacific Northwest National Laboratory), [email protected] Thematic Area(s): (RF07) Hadron Spectroscopy 1 Abstract: The Belle II experiment at the SuperKEKB energy-asymmetric e+e− collider is a substantial upgrade of the B factory facility at KEK in Tsukuba, Japan. -
Discovery Potential for the Lhcb Fully Charm Tetraquark X(6900) State Via P¯P Annihilation Reaction
PHYSICAL REVIEW D 102, 116014 (2020) Discovery potential for the LHCb fully charm tetraquark Xð6900Þ state via pp¯ annihilation reaction † ‡ Xiao-Yun Wang,1,* Qing-Yong Lin,2, Hao Xu,3 Ya-Ping Xie,4 Yin Huang,5 and Xurong Chen4,6,7, 1Department of physics, Lanzhou University of Technology, Lanzhou 730050, China 2Department of Physics, Jimei University, Xiamen 361021, China 3Department of Applied Physics, School of Science, Northwestern Polytechnical University, Xi’an 710129, China 4Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China 5School of Physical Science and Technology, Southwest Jiaotong University, Chendu 610031, China 6University of Chinese Academy of Sciences, Beijing 100049, China 7Guangdong Provincial Key Laboratory of Nuclear Science, Institute of Quantum Matter, South China Normal University, Guangzhou 510006, China (Received 2 August 2020; accepted 16 November 2020; published 18 December 2020) Inspired by the observation of the fully-charm tetraquark Xð6900Þ state at LHCb, the production of Xð6900Þ in pp¯ → J=ψJ=ψ reaction is studied within an effective Lagrangian approach and Breit-Wigner formula. The numerical results show that the cross section of Xð6900Þ at the c.m. energy of 6.9 GeV is much larger than that from the background contribution. Moreover, we estimate dozens of signal events can be detected by the D0 experiment, which indicates that searching for the Xð6900Þ via antiproton-proton scattering may be a very important and promising way. Therefore, related experiments are suggested to be carried out. DOI: 10.1103/PhysRevD.102.116014 I. INTRODUCTION Γ ¼ 168 Æ 33 Æ 69 MeV; ð2Þ In recent decades, more and more exotic hadron states have been observed [1]. -
Detectors for Extreme Luminosity: Belle II
Nuclear Inst. and Methods in Physics Research, A 907 (2018) 46–59 Contents lists available at ScienceDirect Nuclear Inst. and Methods in Physics Research, A journal homepage: www.elsevier.com/locate/nima Detectors for extreme luminosity: Belle II I. Adachi a,b , T.E. Browder c, P. Kriºan d,e, *, S. Tanaka a,b , Y. Ushiroda a,b,f , (on behalf of the Belle II Collaboration) a High Energy Accelerator Research Organization (KEK), Tsukuba, Japan b SOKENDAI (The Graduate University for Advanced Studies), Hayama 240-0193, Japan c University of Hawaii, Honolulu, HI, United States d Faculty of Mathematics and Physics, University of Ljubljana, Slovenia e Joºef Stefan Institute, Ljubljana, Slovenia f Department of Physics, Graduate School of Science, University of Tokyo, Japan ARTICLEINFO ABSTRACT Keywords: We describe the Belle II detector at the SuperKEKB electron–positron accelerator. SuperKEKB operates at the Belle II energy of the 훶 .4S/ resonance where pairs of B mesons are produced in a coherent quantum mechanical state Super B Factory with no additional particles. Belle II, the first Super B factory detector, aims to achieve performance comparable SuperKEKB to the original Belle and BaBar B factory experiments, which first measured the large CP violating effects in the Magnetic spectrometer B meson system, with much higher luminosity collisions and larger beam-induced backgrounds. Flavor physics Contents 1. Introduction ..................................................................................................................................................................................................... -
Front-End Electronic Readout System for the Belle II Imaging Time-Of- Propagation Detector
Front-end electronic readout system for the Belle II imaging Time-Of- Propagation detector Dmitri Kotchetkova, Oskar Hartbricha,*, Matthew Andrewa, Matthew Barretta,1, Martin Bessnera, Vishal Bhardwajb,2, Thomas Browdera, Julien Cercillieuxa, Ryan Conradc, Istvan Dankod, Shawn Dubeya, James Fastc, Bryan Fulsomc, Christopher Kettera, Brian Kirbya,3, Alyssa Loosb, Luca Macchiaruloa, Boštjan Mačeka,4, Kurtis Nishimuraa, Milind Purohitb, Carl Rosenfeldb, Ziru Sanga, Vladimir Savinovd, Gary Varnera, Gerard Vissere, Tobias Webera,5, Lynn Woodc a. Department of Physics and Astronomy, University of Hawaii at Manoa, 2505 Correa Road, Honolulu, HI 96822, USA b. Department of Physics and Astronomy, University of South Carolina, 712 Main Street, Columbia, SC 29208, USA c. Pacific Northwest National Laboratory, 902 Battelle Boulevard, Richland, WA 99354, USA d. Department of Physics and Astronomy, University of Pittsburgh, 3941 O’Hara Street, Pittsburgh, PA 15260, USA e. Center for Exploration of Energy and Matter, Indiana University, 2401 North Milo B. Sampson Lane, Bloomington, IN 47408, USA * Corresponding author. Phone: 1-808-956-4097. Fax: 1-808-956-2930 E-mail address: [email protected] 1Present address: Department of Physics and Astronomy, Wayne State University, 666 W Hancock St, Detroit, MI 48201, USA 2Present address: Indian Institute of Science Education and Research Mohali, Knowledge city, Sector 81, SAS Nagar, Manauli PO 140306, India 3Present address: Physics Department, Brookhaven National Laboratory, Upton, NY 11973, USA 4Present address: Department of Experimental Particle Physics, Jožef Stefan Institute, Jamova cesta 39, 1000 Ljubljana, Slovenia 5Present address: Ruhr-Universität Bochum, 44780 Bochum, Germany Abstract The Time-Of-Propagation detector is a Cherenkov particle identification detector based on quartz radiator bars for the Belle II experiment at the SuperKEKB e+e– collider. -
Observation of Structure in the J/Ψ-Pair Mass Spectrum
EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH (CERN) CERN-EP-2020-115 LHCb-PAPER-2020-011 CERN-EP-2020-115June 30, 2020 22 June 2020 Observation of structure in the J= -pair mass spectrum LHCb collaborationy Abstract p Using proton-proton collision data at centre-of-mass energies of s = 7, 8 and 13 TeV recorded by the LHCb experiment at the Large Hadron Collider, corresponding to an integrated luminosity of 9 fb−1, the invariant mass spectrum of J= pairs is studied. A narrow structure around 6:9 GeV/c2 matching the lineshape of a resonance and a broad structure just above twice the J= mass are observed. The deviation of the data from nonresonant J= -pair production is above five standard deviations in the mass region between 6:2 and 7:4 GeV/c2, covering predicted masses of states composed of four charm quarks. The mass and natural width of the narrow X(6900) structure are measured assuming a Breit{Wigner lineshape. Submitted to Science Bulletin c 2020 CERN for the benefit of the LHCb collaboration. CC BY 4.0 licence. yAuthors are listed at the end of this paper. ii 1 1 Introduction 2 The strong interaction is one of the fundamental forces of nature and it governs the 3 dynamics of quarks and gluons. According to quantum chromodynamics (QCD), the 4 theory describing the strong interaction, quarks are confined into hadrons, in agreement 5 with experimental observations. The quark model [1,2] classifies hadrons into conventional 6 mesons (qq) and baryons (qqq or qqq), and also allows for the existence of exotic hadrons 7 such as tetraquarks (qqqq) and pentaquarks (qqqqq). -
The Belle II Experiment: Status and Prospects
universe Article The Belle II Experiment: Status and Prospects Paolo Branchini † INFN Sezione di RomaTre Via Della Vasca Navale, 84, 00146 Roma, Italy; [email protected] † On behalf of the Belle II Collaboration. Received: 16 September 2018; Accepted: 29 September 2018; Published: 1 October2018 Abstract: The Belle II experiment is a substantial upgrade of the Belle detector and will operate at the SuperKEKBenergy-asymmetric e+e− collider. The accelerator has already successfully completed the first phase of commissioning in 2016. The first electron versus positron collisions in Belle II were delivered in April 2018. The design luminosity of SuperKEKB is 8 × 1035 cm−2 s−1, and the Belle II experiment aims to record 50 ab−1 of data, a factor of 50 more than the Belle experiment. This large dataset will be accumulated with low backgrounds and high trigger efficiencies in a clean e+e− environment. This contribution will review the detector upgrade, the achieved detector performance and the plans for the commissioning of Belle II. Keywords: flavor; dark matter 1. Introduction Even though the Standard Model (SM) is currently the best description of the subatomic world, it does not explain the complete picture. The theory incorporates only three out of the four fundamental forces, omitting gravity. Moreover, there are also important questions that it does not answer, such as the matter versus antimatter asymmetry in the number of quark and lepton generations. Many New Physics (NP) scenarios have been proposed. Experiments in high-energy physics search for NP using two complementary approaches. The first, at the energy frontier, is able to discover new particles directly produced in pp collisions (ATLAS, CMS). -
Model-Independent Evidence for Exotic Hadron Contributions To#[Subscript B][Superscript 0]→J/#Pπ−Decays
Model-Independent Evidence for Exotic Hadron Contributions to#[subscript b][superscript 0]→J/#pπ−Decays The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters. Citation Aaij, R., C. Abellán Beteta, B. Adeva, M. Adinolfi, Z. Ajaltouni, S. Akar, J. Albrecht, et al. "Model-Independent Evidence for Exotic Hadron Contributions toΛ[subscript b][superscript 0]→J/ψpπ−Decays." Physical Review Letters 117, 082002 (August 2016): 1-9 © 2016 CERN for the LHCb Collaboration As Published http://dx.doi.org/10.1103/PhysRevLett.117.082002 Publisher American Physical Society Version Final published version Citable link http://hdl.handle.net/1721.1/110294 Terms of Use Creative Commons Attribution Detailed Terms http://creativecommons.org/licenses/by/3.0 week ending PRL 117, 082002 (2016) PHYSICAL REVIEW LETTERS 19 AUGUST 2016 0 − Model-Independent Evidence for J=ψp Contributions to Λb → J=ψpK Decays R. Aaij et al.* (LHCb Collaboration) (Received 19 April 2016; published 18 August 2016) 0 − The data sample of Λb → J=ψpK decays acquired with the LHCb detector from 7 and 8 TeV pp collisions, corresponding to an integrated luminosity of 3 fb−1, is inspected for the presence of J=ψp or J=ψK− contributions with minimal assumptions about K−p contributions. It is demonstrated at more than 0 − − nine standard deviations that Λb → J=ψpK decays cannot be described with K p contributions alone, and that J=ψp contributions play a dominant role in this incompatibility. These model-independent results þ support the previously obtained model-dependent evidence for Pc → J=ψp charmonium-pentaquark states in the same data sample.