Understanding the J/Psi Production Mechanism at PHENIX Todd Kempel Iowa State University
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Production and Hadronization of Heavy Quarks
View metadata, citation and similar papers at core.ac.uk brought to you by CORE LU TP 00–16 provided by CERN Document Server hep-ph/0005110 May 2000 Production and Hadronization of Heavy Quarks E. Norrbin1 and T. Sj¨ostrand2 Department of Theoretical Physics, Lund University, Lund, Sweden Abstract Heavy long-lived quarks, i.e. charm and bottom, are frequently studied both as tests of QCD and as probes for other physics aspects within and beyond the standard model. The long life-time implies that charm and bottom hadrons are formed and observed. This hadronization process cannot be studied in isolation, but depends on the production environment. Within the framework of the string model, a major effect is the drag from the other end of the string that the c/b quark belongs to. In extreme cases, a small-mass string can collapse to a single hadron, thereby giving a non- universal flavour composition to the produced hadrons. We here develop and present a detailed model for the charm/bottom hadronization process, involving the various aspects of string fragmentation and collapse, and put it in the context of several heavy-flavour production sources. Applications are presented from fixed-target to LHC energies. [email protected] [email protected] 1 Introduction The light u, d and s quarks can be obtained from a number of sources: valence flavours in hadronic beam particles, perturbative subprocesses and nonperturbative hadronization. Therefore the information carried by identified light hadrons is highly ambiguous. The charm and bottom quarks have masses significantly above the ΛQCD scale, and therefore their production should be perturbatively calculable. -
Studies of Hadronization Mechanisms Using Pion Electroproduction in Deep Inelastic Scattering from Nuclei
Studies of Hadronization Mechanisms using Pion Electroproduction in Deep Inelastic Scattering from Nuclei Will Brooks, Hayk Hakobyan, Cristian Peña, Miguel Arratia Universidad Técnica Federico Santa María Valparaíso, Chile for the CLAS collaboration related posters: π0, T. Mineeva; Σ-, G. & I. Niculescu • Goal: study space-time properties of parton propagation and fragmentation in QCD: • Characteristic timescales • Hadronization mechanisms • Partonic energy loss • Use nuclei as spatial filters with known properties: • size, density, interactions • Unique kinematic window at low energies Comparison of Parton Propagation in Three Processes DIS D-Y RHI Collisions Accardi, Arleo, Brooks, d'Enterria, Muccifora Riv.Nuovo Cim.032:439553,2010 [arXiv:0907.3534] Majumder, van Leuween, Prog. Part. Nucl. Phys. A66:41, 2011, arXiv:1002.2206 [hep- ph] Deep Inelastic Scattering - Vacuum tp h tf production time tp - propagating quark h formation time tf - dipole grows to hadron partonic energy loss - dE/dx via gluon radiation in vacuum Low-Energy DIS in Cold Nuclear Medium Partonic multiple scattering: medium-stimulated gluon emission, broadened pT Low-Energy DIS in Cold Nuclear Medium Partonic multiple scattering: medium-stimulated gluon emission, broadened pT Hadron forms outside the medium; or.... Low-Energy DIS in Cold Nuclear Medium Hadron can form inside the medium; then also have prehadron/hadron interaction Low-Energy DIS in Cold Nuclear Medium Hadron can form inside the medium; then also have prehadron/hadron interaction Amplitudes for hadronization -
Effective Field Theories for Quarkonium
Effective Field Theories for Quarkonium recent progress Antonio Vairo Technische Universitat¨ Munchen¨ Outline 1. Scales and EFTs for quarkonium at zero and finite temperature 2.1 Static energy at zero temperature 2.2 Charmonium radiative transitions 2.3 Bottomoniun thermal width 3. Conclusions Scales and EFTs Scales Quarkonia, i.e. heavy quark-antiquark bound states, are systems characterized by hierarchies of energy scales. These hierarchies allow systematic studies. They follow from the quark mass M being the largest scale in the system: • M ≫ p • M ≫ ΛQCD • M ≫ T ≫ other thermal scales The non-relativistic expansion • M ≫ p implies that quarkonia are non-relativistic and characterized by the hierarchy of scales typical of a non-relativistic bound state: M ≫ p ∼ 1/r ∼ Mv ≫ E ∼ Mv2 The hierarchy of non-relativistic scales makes the very difference of quarkonia with heavy-light mesons, which are just characterized by the two scales M and ΛQCD. Systematic expansions in the small heavy-quark velocity v may be implemented at the Lagrangian level by constructing suitable effective field theories (EFTs). ◦ Brambilla Pineda Soto Vairo RMP 77 (2004) 1423 Non-relativistic Effective Field Theories LONG−RANGE SHORT−RANGE Caswell Lepage PLB 167(86)437 QUARKONIUM QUARKONIUM / QED ◦ ◦ Lepage Thacker NP PS 4(88)199 QCD/QED ◦ Bodwin et al PRD 51(95)1125, ... M perturbative matching perturbative matching ◦ Pineda Soto PLB 420(98)391 µ ◦ Pineda Soto NP PS 64(98)428 ◦ Brambilla et al PRD 60(99)091502 Mv NRQCD/NRQED ◦ Brambilla et al NPB 566(00)275 ◦ Kniehl et al NPB 563(99)200 µ ◦ Luke Manohar PRD 55(97)4129 ◦ Luke Savage PRD 57(98)413 2 non−perturbative perturbative matching Mv matching ◦ Grinstein Rothstein PRD 57(98)78 ◦ Labelle PRD 58(98)093013 ◦ Griesshammer NPB 579(00)313 pNRQCD/pNRQED ◦ Luke et al PRD 61(00)074025 ◦ Hoang Stewart PRD 67(03)114020, .. -
Quarkonium Interactions in QCD1
CERN-TH/95-342 BI-TP 95/41 Quarkonium Interactions in QCD1 D. KHARZEEV Theory Division, CERN, CH-1211 Geneva, Switzerland and Fakult¨at f¨ur Physik, Universit¨at Bielefeld, D-33501 Bielefeld, Germany CONTENTS 1. Introduction 1.1 Preview 1.2 QCD atoms in external fields 2. Operator Product Expansion for Quarkonium Interactions 2.1 General idea 2.2 Wilson coefficients 2.3 Sum rules 2.4 Absorption cross sections 3. Scale Anomaly, Chiral Symmetry and Low-Energy Theorems 3.1 Scale anomaly and quarkonium interactions 3.2 Low energy theorem for quarkonium interactions with pions 3.3 The phase of the scattering amplitude 4. Quarkonium Interactions in Matter 4.1 Nuclear matter 4.2 Hadron gas 4.3 Deconfined matter 5. Conclusions and Outlook 1Presented at the Enrico Fermi International School of Physics on “Selected Topics in Non-Perturbative QCD”, Varenna, Italy, June 1995; to appear in the Proceedings. 1 Introduction 1.1 Preview Heavy quarkonia have proved to be extremely useful for understanding QCD. The large mass of heavy quarks allows a perturbation theory analysis of quarkonium decays [1] (see [2] for a recent review). Perturbation theory also provides a rea- sonable first approximation to the correlation functions of quarkonium currents; deviations from the predictions of perturbation theory can therefore be used to infer an information about the nature of non-perturbative effects. This program was first realized at the end of the seventies [3]; it turned out to be one of the first steps towards a quantitative understanding of the QCD vacuum. The natural next step is to use heavy quarkonia to probe the properties of excited QCD vacuum, which may be produced in relativistic heavy ion collisions; this was proposed a decade ago [4]. -
J. Stroth Asked the Question: "Which Are the Experimental Evidences for a Long Mean Free Path of Phi Mesons in Medium?"
J. Stroth asked the question: "Which are the experimental evidences for a long mean free path of phi mesons in medium?" Answer by H. Stroebele ~~~~~~~~~~~~~~~~~~~ (based on the study of several publications on phi production and information provided by the theory friends of H. Stöcker ) Before trying to find an answer to this question, we need to specify what is meant with "long". The in medium cross section is equivalent to the mean free path. Thus we need to find out whether the (in medium) cross section is large (with respect to what?). The reference would be the cross sections of other mesons like pions or more specifically the omega meson. There is a further reference, namely the suppression of phi production and decay described in the OZI rule. A “blind” application of the OZI rule would give a cross section of the phi three orders of magnitude lower than that of the omega meson and correspondingly a "long" free mean path. In the following we shall look at the phi production cross sections in photon+p, pion+p, and p+p interactions. The total photoproduction cross sections of phi and omega mesons were measured in a bubble chamber experiment (J. Ballam et al., Phys. Rev. D 7, 3150, 1973), in which a cross section ratio of R(omega/phi) = 10 was found in the few GeV beam energy region. There are results on omega and phi production in p+p interactions available from SPESIII (Near- Threshold Production of omega mesons in the Reaction p p → p p omega", Phys.Rev.Lett. -
Monte Carlo Methods in Particle Physics Bryan Webber University of Cambridge IMPRS, Munich 19-23 November 2007
Monte Carlo Methods in Particle Physics Bryan Webber University of Cambridge IMPRS, Munich 19-23 November 2007 Monte Carlo Methods 3 Bryan Webber Structure of LHC Events 1. Hard process 2. Parton shower 3. Hadronization 4. Underlying event Monte Carlo Methods 3 Bryan Webber Lecture 3: Hadronization Partons are not physical 1. Phenomenological particles: they cannot models. freely propagate. 2. Confinement. Hadrons are. 3. The string model. 4. Preconfinement. Need a model of partons' 5. The cluster model. confinement into 6. Underlying event hadrons: hadronization. models. Monte Carlo Methods 3 Bryan Webber Phenomenological Models Experimentally, two jets: Flat rapidity plateau and limited Monte Carlo Methods 3 Bryan Webber Estimate of Hadronization Effects Using this model, can estimate hadronization correction to perturbative quantities. Jet energy and momentum: with mean transverse momentum. Estimate from Fermi motion Jet acquires non-perturbative mass: Large: ~ 10 GeV for 100 GeV jets. Monte Carlo Methods 3 Bryan Webber Independent Fragmentation Model (“Feynman—Field”) Direct implementation of the above. Longitudinal momentum distribution = arbitrary fragmentation function: parameterization of data. Transverse momentum distribution = Gaussian. Recursively apply Hook up remaining soft and Strongly frame dependent. No obvious relation with perturbative emission. Not infrared safe. Not a model of confinement. Monte Carlo Methods 3 Bryan Webber Confinement Asymptotic freedom: becomes increasingly QED-like at short distances. QED: + – but at long distances, gluon self-interaction makes field lines attract each other: QCD: linear potential confinement Monte Carlo Methods 3 Bryan Webber Interquark potential Can measure from or from lattice QCD: quarkonia spectra: String tension Monte Carlo Methods 3 Bryan Webber String Model of Mesons Light quarks connected by string. -
Fragmentation and Hadronization 1 Introduction
Fragmentation and Hadronization Bryan R. Webber Theory Division, CERN, 1211 Geneva 23, Switzerland, and Cavendish Laboratory, University of Cambridge, Cambridge CB3 0HE, U.K.1 1 Introduction Hadronic jets are amongst the most striking phenomena in high-energy physics, and their importance is sure to persist as searching for new physics at hadron colliders becomes the main activity in our field. Signatures involving jets almost always have the largest cross sections, but are the most difficult to interpret and to distinguish from background. Insight into the properties of jets is therefore doubly valuable: both as a test of our understanding of strong interaction dy- namics and as a tool for extracting new physics signals in multi-jet channels. In the present talk, I shall concentrate on jet fragmentation and hadroniza- tion, the topic of jet production having been covered admirably elsewhere [1, 2]. The terms fragmentation and hadronization are often used interchangeably, but I shall interpret the former strictly as referring to inclusive hadron spectra, for which factorization ‘theorems’2 are available. These allow predictions to be made without any detailed assumptions concerning hadron formation. A brief review of the relevant theory is given in Section 2. Hadronization, on the other hand, will be taken here to refer specifically to the mechanism by which quarks and gluons produced in hard processes form the hadrons that are observed in the final state. This is an intrinsically non- perturbative process, for which we only have models at present. The main models are reviewed in Section 3. In Section 4 their predictions, together with other less model-dependent expectations, are compared with the latest data on single- particle yields and spectra. -
Strange Hadrocharmonium ∗ M.B
Physics Letters B 798 (2019) 135022 Contents lists available at ScienceDirect Physics Letters B www.elsevier.com/locate/physletb Strange hadrocharmonium ∗ M.B. Voloshin a,b,c, a William I. Fine Theoretical Physics Institute, University of Minnesota, Minneapolis, MN 55455, USA b School of Physics and Astronomy, University of Minnesota, Minneapolis, MN 55455, USA c Institute of Theoretical and Experimental Physics, Moscow, 117218, Russia a r t i c l e i n f o a b s t r a c t Article history: It has been recently suggested that the charged charmoniumlike resonances Zc (4100) and Zc (4200) Received 23 May 2019 are two states of hadrocharmonium, related by the charm quark spin symmetry in the same way Received in revised form 12 August 2019 as the lowest charmonium states ηc and J/ψ. It is pointed out here that in this picture one might Accepted 16 September 2019 expect existence of their somewhat heavier strange counterparts, Zcs, decaying to ηc K and J/ψ K . Some Available online 11 October 2019 expected properties of such charmoniumlike strange resonances are discussed that set benchmarks for Editor: B. Grinstein their search in the decays of the strange Bs mesons. © 2019 The Author. Published by Elsevier B.V. This is an open access article under the CC BY license 3 (http://creativecommons.org/licenses/by/4.0/). Funded by SCOAP . Numerous new resonances recently uncovered near the open down to about 4220 MeV), has been recently invoked [11]for de- charm and open bottom thresholds, the so-called XYZ states, ap- scription of the charged charmoniumlike resonances Zc(4100) and parently do not fit in the standard quark-antiquark template and Zc(4200) observed respectively in the decay channels ηcπ [12] 1 contain light constituents in addition to a heavy quark-antiquark and J/ψπ [13]. -
Hadronization from the QGP in the Light and Heavy Flavour Sectors Francesco Prino INFN – Sezione Di Torino Heavy-Ion Collision Evolution
Hadronization from the QGP in the Light and Heavy Flavour sectors Francesco Prino INFN – Sezione di Torino Heavy-ion collision evolution Hadronization of the QGP medium at the pseudo- critical temperature Transition from a deconfined medium composed of quarks, antiquarks and gluons to color-neutral hadronic matter The partonic degrees of freedom of the deconfined phase convert into hadrons, in which partons are confined No first-principle description of hadron formation Non-perturbative problem, not calculable with QCD → Hadronisation from a QGP may be different from other cases in which no bulk of thermalized partons is formed 2 Hadron abundances Hadron yields (dominated by low-pT particles) well described by statistical hadronization model Abundances follow expectations for hadron gas in chemical and thermal equilibrium Yields depend on hadron masses (and spins), chemical potentials and temperature Questions not addressed by the statistical hadronization approach: How the equilibrium is reached? How the transition from partons to hadrons occurs at the microscopic level? 3 Hadron RAA and v2 vs. pT ALICE, PRC 995 (2017) 064606 ALICE, JEP09 (2018) 006 Low pT (<~2 GeV/c) : Thermal regime, hydrodynamic expansion driven by pressure gradients Mass ordering High pT (>8-10 GeV/c): Partons from hard scatterings → lose energy while traversing the QGP Hadronisation via fragmentation → same RAA and v2 for all species Intermediate pT: Kinetic regime, not described by hydro Baryon / meson grouping of v2 Different RAA for different hadron species -
On the Scent of Glue
On the scent of glue by Frank Close Although this work was not new Soon after the quark model was in has been intensifying over the last for the specialists, the underlying vented twenty years ago, people re several years. Where have all the message was clear. 'Because of its alized that it was in trouble. The Pauli flowers gone? inherent singularities, classical gen exclusion principle ruled out many eral relativity predicts its own down well known states, in particular the How colour forces work fall,' stated Hawking, 'just as the configuration of three identical classical picture of the atom was also strange quarks that formed the ome Electrical charges are the sources doomed'. ga-minus. The very hadron whose of electromagnetic forces. As every The meeting merited two closing discovery had confirmed the Eight schoolchild knows, opposite char lectures. For the cosmologists, Mar fold Way seemingly killed its off ges attract while like charges repel. tin Rees of Cambridge confessed to spring, the quark model. Quarks possess electric charge and finding the symposium an 'unusual In those days, many people were so feel electromagnetic forces. That experience'. For the particle physi reluctant to accept the idea of frac is why even electrically uncharged cists, John Ellis described particle tionally charged quarks which had particles like neutrons have electro physics and cosmology as having 'a never been seen. The Pauli paradox magnetic interactions; they contain brilliant past in front of them' — refer suggested that quarks were at best electrically charged constituents. ring to the new common interest in no more than a bookkeeping device, Quarks also have colour and it ap the primaeval Big Bang and its imme not physical particles. -
Kaon to Two Pions Decays from Lattice QCD: ∆I = 1/2 Rule and CP
Kaon to Two Pions decays from Lattice QCD: ∆I =1/2 rule and CP violation Qi Liu Submitted in partial fulfillment of the requirements for the degree of Doctor of Philosophy in the Graduate School of Arts and Sciences COLUMBIA UNIVERSITY 2012 c 2012 Qi Liu All Rights Reserved Abstract Kaon to Two Pions decays from Lattice QCD: ∆I =1/2 rule and CP violation Qi Liu We report a direct lattice calculation of the K to ππ decay matrix elements for both the ∆I = 1/2 and 3/2 amplitudes A0 and A2 on a 2+1 flavor, domain wall fermion, 163 32 16 lattice ensemble and a 243 64 16 lattice ensemble. This × × × × is a complete calculation in which all contractions for the required ten, four-quark operators are evaluated, including the disconnected graphs in which no quark line connects the initial kaon and final two-pion states. These lattice operators are non- perturbatively renormalized using the Rome-Southampton method and the quadratic divergences are studied and removed. This is an important but notoriously difficult calculation, requiring high statistics on a large volume. In this work we take a major step towards the computation of the physical K ππ amplitudes by performing → a complete calculation at unphysical kinematics with pions of mass 422MeV and 329MeV at rest in the kaon rest frame. With this simplification we are able to 3 resolve Re(A0) from zero for the first time, with a 25% statistical error on the 16 3 lattice and 15% on the 24 lattice. The complex amplitude A2 is calculated with small statistical errors. -
Effective Field Theories of Heavy-Quark Mesons
Effective Field Theories of Heavy-Quark Mesons A thesis submitted to The University of Manchester for the degree of Doctor of Philosophy (PhD) in the faculty of Engineering and Physical Sciences Mohammad Hasan M Alhakami School of Physics and Astronomy 2014 Contents Abstract 10 Declaration 12 Copyright 13 Acknowledgements 14 1 Introduction 16 1.1 Ordinary Mesons......................... 21 1.1.1 Light Mesons....................... 22 1.1.2 Heavy-light Mesons.................... 24 1.1.3 Heavy-Quark Mesons................... 28 1.2 Exotic cc¯ Mesons......................... 31 1.2.1 Experimental and theoretical studies of the X(3872). 34 2 From QCD to Effective Theories 41 2.1 Chiral Symmetry......................... 43 2.1.1 Chiral Symmetry Breaking................ 46 2.1.2 Effective Field Theory.................. 57 2.2 Heavy Quark Spin Symmetry.................. 65 2.2.1 Motivation......................... 65 2.2.2 Heavy Quark Effective Theory.............. 69 3 Heavy Hadron Chiral Perturbation Theory 72 3.1 Self-Energies of Charm Mesons................. 78 3.2 Mass formula for non-strange charm mesons.......... 89 3.2.1 Extracting the coupling constant of even and odd charm meson transitions..................... 92 2 4 HHChPT for Charm and Bottom Mesons 98 4.1 LECs from Charm Meson Spectrum............... 99 4.2 Masses of the charm mesons within HHChPT......... 101 4.3 Linear combinations of the low energy constants........ 106 4.4 Results and Discussion...................... 108 4.5 Prediction for the Spectrum of Odd- and Even-Parity Bottom Mesons............................... 115 5 Short-range interactions between heavy mesons in frame- work of EFT 126 5.1 Uncoupled Channel........................ 127 5.2 Two-body scattering with a narrow resonance........