Perspectives with PANDA. The new accelerator complex of GSI The antiproton s s activity The PANDA scientific program Paola Gianotti LNF
|
|
- Grace Gibbs
- 5 years ago
- Views:
Transcription
1 Perspectives with PANDA The new accelerator complex of GSI The antiproton s s activity The PANDA scientific program Paola Gianotti LNF
2 FAIR The GSI future facility FAIR Facility for Antiproton and Ion Research SIS UNILAC SIS 100/300 Primary Beams /s; 1.5 GeV/u; 238 U 28+ Factor present in intensity 2(4)x10 13 /s 30 GeV protons /s 238 U 73+ up to 25 (- 35) GeV/u FRS ESR CBM Secondary Beams PP Atomic Physics p Target Super FRS HESR PANDA Broad range of radioactive beams up to GeV/u; up to factor in intensity over present Antiprotons 3 (0) - 30 GeV CR + RESR Key Technical Features NESR FLAIR Cooled beams Rapidly cycling superconducting magnets Storage and Cooler Rings Radioactive beams e A collider stored and cooled GeV antiprotons
3 HESR - High Energy Storage Ring Production rate 2x10 7 /sec P beam N stored = 1-15 GeV/c _ = 5x10 10 p Internal Target High luminosity mode High resolution mode Lumin. = 2 x cm 2 s 1 δp/p ~ 10 4 (stochastic cooling) δp/p ~ 10 5 (electron cooling) Lumin. = cm 2 s 1
4 Summary of Research Areas at the GSI Future Facility Structure and Dynamics of Nuclei - Radioactive Beams Nucleonic matter Nuclear astrophysics Fundamental symmetries Hadron Structure and Quark-Gluon Dynamics - Antiprotons Non-pertubative QCD Quark-gluon degrees of freedom Confinement and chiral symmetry Hypernuclear physics Nuclear Matter and the Quark-Gluon Plasma - Relativistic HI - Beams Physics of Dense Plasmas and Bulk Matter - Bunch Compression Properties of high density plasmas Phase transitions and equation of state Laser - ion interaction with and in plasmas Temperature [ev] Nuclear phase diagram Compressed nuclear/strange matter Deconfinement and chiral symmetry Magnetic Fusion Inertial Cofinement Fusion Sun Core PHELIX Laser Heating as sm led up pla al co Ide gly as on sm Ion Beam Str pla Heating SIS 18 Sun Surface Density [cm-3] Ultra High EM-Fields and Applications - Ions & Petawatt Laser QED and critical fields Ion - laser interaction Ion - matter interaction solid state density Jupiter
5 Antiproton Physics Program Charmonium ( cc ) spectroscopy: precision measurements of mass, width, decay branches of all charmonium states, especially for extracting information on the quark confinement. Search for gluonic excitations (charmed hybrids, glueballs) in the charmonium mass range (3 5 GeV/c 2 ). Search for modifications of meson properties in the nuclear medium, and their possible relationship to the partial restoration of chiral symmetry for light quarks. Precision γ-ray spectroscopy of single and double hypernuclei for Extracting information on their structure and on the hyperon-nucleon and hyperon-hyperon interaction. Inverted DVCS to extract parton distributions. Proton form-factors at large Q 2 up to 25 GeV 2 /c 4. D-meson decay spectroscopy BR and decay dalitz plots CP-Violation in the D/Λ sector.
6 Charmonium Physics e + e Ψ γχ 1,2 γγj/ψ γγe + e _ p p χ 1,2 γj/ψ γe+ e e+e interactions: - Only 1 states are formed - Other states only by secondary decays (moderate mass resolution) _ pp reactions: - All states directly formed (very good mass resolution) _ Br( pp η c ) = CBall ev./2 MeV χ c MeV CBall E835 Br(e + e ψ) Br(ψ γη c ) = E 835 ev./pb E CM
7 Charmonium Physics Charmonium spectrum, glueballs, spin-exotics cc-glue cc-glue hybrids hybrids with with experimental results results m r 0 2S+1 LJ 1 S0 3 S1 1 P1 3 P0 3 P1 3 P2 1 D2 3 D2 3 D3 1 F3 3 F3 n.a η c J/Ψ h c χc0 χ c1 χ c2 experiment DD ** DD CP PACS Columbia hybrids glueballs J PC exotic From G.S. Bali, Eur. Phys. J A 19 (2004) m/gev?(3943) enancement in J/Ψω mass spectrum X(3872) first seen by Belle Then confirmed by others B-factories are abundant sources of data on charmonium
8 Mass η c ±1.2 Decay channels studied Total BR seen (%) Decay Channels With error <30% η c ±6.0 4 ~ 0 0 J/ψ ± ψ ± χ c ± χ c ± χ c ± h c 2? 0 ψ (3770) ±2.4 2 ~ 0 1 ψ (3836) 3836±13 1 ~ 0 0 X(3872) ±0.6 3 ~ 0 0 ψ (4040) 4040±10 6 ~0 1 ψ (4160) 4159±20 1 ~0 0 ψ (4415) 4415±6 2 ~0 0
9 Exotic hadrons The QCD spectrum is much rich than that of the naive quark model also the gluons can act as hadron components The exotic hadrons fall in 3 general categories: Multiquarks (qq)(qq) Hybrids Glueballs (qq) g gg Exotic light qq Exotic cc MeV/c 2 In the cc meson spectrum the density of states is lower and therefore the overlap
10 Exotic hadrons In the light meson region, about 10 states have been classified as Exotics. Almost all of them have been seen in pp... f 0 (980) f 0 (1500) f 0 (1370) f 0 (1710) η(1410); η(1460) f 1 (1420) Main non-qq candidates 4q state 0 ++ glueball candidate 0 ++ glueball candidate 0 ++ glueball candidate 0 + glueball candidate hybrid, 4q state π 1 (1400) hybrid candidate 1 + π 1 (1600) hybrid candidate 1 + π (1800) hibrid candidate 0 + π 2 (1900) hybrid candidate 2 + π 1 (2000) hybrid candidate 1 + a 2 (2100) hybrid candidate 1 ++
11 Charmed Hybrids Flux tube-model predicts H DD** (+c.c.) decays If m H <4290 MeV/c 2 Γ H < 50 MeV/c 2 Gluonic excitations of the quark-antiquark-potential may lead to bound states LQCD: r 0 =0.5fm Some exotics can decay neither to DD nor to DD*+c.c. e.g.: J PC (H)=0 +- Flux-tube allowed χ c0 ω,χ c0 φ,χ c2 ω,χ c2 φ, η c, h 1, h 1c η Flux-tube forbidden J/ψf 2,J/ψ(ππ) S Small number of final states with small phase space m H ~ GeV ; J PC 1 -+
12 Mesons in nuclear matter One of the fundamental question of QCD is the generation of MASS The light meson masses are larger than the sum of the constituent quark masses! Spontaneous chiral symmetry breaking seems to play a decisive role in the mass generation of light mesons. How can we check this?
13 Hadrons in nuclear matter Since density increase in nuclear matter is possible a partial restoration of chiral symmetry Light quarks are sensitive to quark condensate Evidence for mass changes of pions and kaons has been observed Deeply bound pionic atoms Kaon-production environments Proton-Proton Collisions Nucleus-Nucleus Collisions f* π = 0.78f π K - K - K + K +
14 Mesons in nuclear matter Mass modifications of mesons With p beam up to 15GeV/c these studies will be extended Sub-threshold enhancement for D and D meson production expected signal: strong enhancement of the D-meson cross section, relative D + D - yields, in the near/sub-threshold region. pionic atoms π KAOS/FOPI K π - 25 MeV π + K MeV σ(nb) D - D + pp D + D - in-medium free masses D HESR vacuum K - D - 50 MeV D + nuclear medium ρ = ρ T (GeV)
15 Mesons in nuclear matter The lowering of the DD thresh. allow Ψ,χ c2 charmonium states to decay into this channel thus resulting in a substantial increase of width of these states states above DD thresh. would have larger width Idea Study relative changes of yield and width of the charmonium state Ψ(3770). BR into l + l (10-5 in free space) GeV/c Mass ψ(1 3 D 1 ) η c (1 1 S 0 ) ψ(3 3 S 1 ) ψ(2 3 S 1 ) χ c2 (1 3 P 2 ) χ c1 (1 3 P 1 ) χ c1 (1 3 P 0 ) ψ(1 3 S 1 ) DD 3,74 vacuum 3,64 1ρ 0 3,54 2ρ 0 Predictions by Ye.S. Golubeva et al., Eur.Phys.J. A 17,(2003)275
16 Other physics topics Reversed Deeply Virtual Compton Scattering and Drell-Yan processes CP-violation (D/Λ sector) -D 0 D 0 mixing SM prediction < compare angular decay asymmetries for ΛΛ SM prediction ~ Rare D-decays: D + µ + ν (BR 10-4 ) Cross section σ s 10 GeV 2 L = cm-2 s events per month c d W + µ + ν
17 Other physics topics Electromagnetic Form Factors of the Proton in the Time-Like Region from threshold up to 20 GeV 2 /c 4 Precise measurement of cross-sections for neutrino factory design
18 QCD systems to be studied at PANDA
19 General Purpose Detector Detector requests: nearly 4π solid angle (partial wave analysis) high rate capability ( annihilations/s) good PID (γ, e,µ, π, K, p) momentum resolution (~1%) vertex info for D, K 0 S, Λ (c τ = 317 µm for D ± ) efficient trigger (e, µ, K, D, Λ) modular design (Hypernuclei experiments)
20 PANDA Detector (top view) DIRC: Detecting Internally Reflected Cherenkov light target spectrometer straw tube tracker mini drift chambers muon counter forward spectrometer iron yoke Solenoidal magnet electromagnetic calorimeter micro vertex detector Length: ~2 m upstream, ~10 m downstream
21 Summary A new new Hadron-Facility is is underway in in Europe: FAIR GSI GSI A wide wide experimetal physics program going going from from meson meson spectroscopy to to hypernuclear physics etc. etc. will will be be accessible with with the the new new GSI GSI antiproton beam beam New New and and interesting results results will will come come in in many many fields fields thanks thanks to to the the unprecedent characteristics of of the the beam beam and and to to the the potentiality of of the the PANDA general porpose detector
PANDA. antiproton Annihilation at DArmstadt
antiproton Annihilation at DArmstadt Physics programme Quark confinement: Charmonium spectroscopy Excited gluons: Exotic hybrid mesons & glueballs Nucleon spin puzzle: transverse quark spin distribution
More informationExperimental overview of the PANDA experiment
Experimental overview of the PANDA experiment Elisa Fioravanti for the PANDA Collaboration INFN Ferrara, Via Saragat 1, 44100 Ferrara, Italy E-mail: fioravanti@fe.infn.it Abstract. The physics program
More informationInternational Workshop on Heavy Quarkonium Oct. 2007, DESY Hamburg. Prospects for Panda. Charmonium Spectroscopy
International Workshop on Heavy Quarkonium 17 20 Oct. 2007, DESY Hamburg Prospects for Panda Charmonium Spectroscopy M. Pelizäus (Ruhr Universität Bochum) for the Panda Collaboration 1 FAIR accelerator
More informationCharmonium Physics with PANDA at FAIR. FZ-Juelich & Uni Bochum
Charmonium Physics with PANDA at FAIR Contents Overview of PANDA Physics program Charmonium Physics Issues with PANDA FAIR Accelerator Facility PANDA Detector Summary Hadron Structure with Precision Measurements
More informationThe PANDA experiment: Antiproton physics at FAIR
IL NUOVO CIMENTO Vol. 34 C, N. 6 Novembre-Dicembre 2011 DOI 10.1393/ncc/i2011-11089-2 Colloquia: IFAE 2011 The PANDA experiment: Antiproton physics at FAIR P. Montagna on behalf of the PANDA Collaboration
More informationAntiproton Physics (Overview of the PANDA Physics Program)
Antiproton Physics (Overview of thepanda Physics Program) Diego Bettoni INFN, Ferrara, Italy International School of Nuclear Physics, From Quarks and Gluons to Hadrons and Nuclei Erice, Italy, 16-24 September
More informationMonte Carlo Simulations for PANDA
Monte Carlo Simulations for PANDA Diego Bettoni Istituto Nazionale di Fisica Nucleare, Ferrara International Workshop on Heavy Quarkonia 2008 Nara, Japan, 3 December 2008 Outline Introduction The PANDA
More informationThe PANDA experiment at FAIR
The PANDA experiment at FAIR Helmholtz-Institut Mainz, Germany On behalf of the PANDA collaboration Facility for Antiproton and Ion Research (FAIR) PANDA physics program PANDA spectrometer PANDA phases
More informationVol. 5 (2012) Acta Physica Polonica B Proceedings Supplement No 4 PANDA AT FAIR. Tord Johansson. representing the PANDA Collaboration
Vol. 5 (2012) Acta Physica Polonica B Proceedings Supplement No 4 PANDA AT FAIR Tord Johansson representing the PANDA Collaboration Departmet of Physics and Astronomy, Uppsala University Box 516, 75120
More informationThe PANDA experiment at FAIR
The PANDA experiment at FAIR Ulrich Wiedner Uppsala University Elba, June 7, 2004 The key issues creation of mass QCD exotics (glueballs, hybrids) charmed hadrons in nuclei confinement exotics states of
More informationPhysics with PANDA at FAIR
Physics with PANDA at FAIR Inti Lehmann University of Glasgow Tbilisi, Sept. 5th, 2006 Some Open Questions in generation of hadron masses spin puzzle Non-Perturbative QCD strong interaction at large distances
More informationPANDA FAIR. Anastasios Belias for the PANDA Collaboration GSI, Darmstadt, Germany. EXA2017, Vienna September 15th, 2017
PANDA Physics @ FAIR Anastasios Belias for the PANDA Collaboration GSI, Darmstadt, Germany EXA2017, Vienna September 15th, 2017 PANDA Physics @ FAIR The Facility PANDA Physics Goals Status & Outlook Facility
More informationHadron Physics with Antiprotons
Hadron Physics with Antiprotons Introduction HESR/PANDA - Project at GSI ( W. Henning) Merits of experiments with antiprotons Physics Program Charmonium Spectroscopy ( D. Bettoni) Heavier Glueballs and
More informationPhysics Goals of PANDA
Physics Goals of PANDA Introduction The PANDA Project PANDA and HESR Status of the PANDA Project Physics Program of PANDA Hadron Spectroscopy Merits of Antiproton Physics Properties of Hadrons in Matter
More informationKärnfysikermötet, Umeå 1-2 November 2005 Agnes Lundborg, Uppsala Universitet
Charmonium in e + e and pp Kärnfysikermötet, Umeå 1-2 November 2005 Agnes Lundborg, Uppsala Universitet Raise a whole bunch of Questions Charmonium is a good tool for QCD studies: Why we want to understand
More informationHADRON PHYSICS WITH ANTI-PROTONS: The PANDA EXPERIMENT AT FAIR
MENU 2007 11th International Conference on Meson-Nucleon Physics and the Structure of the Nucleon September10-14, 2007 IKP, Forschungzentrum Jülich, Germany HADRON PHYSICS WITH ANTI-PROTONS: The PANDA
More informationMilano Fisica conantiprotoni al progetto FAIR del GSI
Milano 4.5.05 Fisica conantiprotoni al progetto FAIR del GSI Present GSI Facility Accelerator Parameters Energies: Unilac < 20 MeV/u SIS 1-2 GeV/u ESR < 0.8 GeV/u SIS UNILAC 3 Injectors HSI: 8 ma Ar 1+
More informationThe PANDA experiment at FAIR
The PANDA experiment at FAIR Diego Bettoni Istituto Nazionale di Fisica Nucleare, Ferrara representing the PANDA collaboration Charm 2007 Cornell University, 8 August 2007 Outline FAIR HESR PANDA Physics
More informationNuclear and Hadron Physics with Antiprotons
Nuclear and Hadron Physics with Antiprotons PANDA @ FAIR Olaf N. Hartmann INFN Laboratori Nazionali di Frascati Overview The Facility: FAIR, HESR The Physics Program The Detector The Collaboration Outlook
More informationThe PANDA Experiment at FAIR
The PANDA Experiment at FAIR Diego Bettoni INFN, Ferrara, Italy Hadrons from Quarks and Gluons Hirschegg, Kleinwalsertal, Austria, January 12-18, 2014 Outline Introduction The FAIR facility Experimental
More informationarxiv: v1 [hep-ex] 30 Oct 2007
Proceedings of the CHARM 2007 Workshop, Ithaca, NY, August 5-8, 2007 1 The PANDA Experiment at FAIR Diego Bettoni Istituto Nazionale di Fisica Nucleare, 44100 Ferrara, Italy The physics program of the
More informationPANDA Experiment. Nordic Winter Meeting on FAIR Björkliden Department of Physics and Astronomy Uppsala University
Department of Physics and Astronomy Uppsala University Nordic Winter Meeting on Phyics @ FAIR Björkliden 1-3-6 1 3 pp Λ c Λ + c 4 5 pp ȲY What are the relevant degrees of freedom to describe a process?
More informationThe PANDA Detector at FAIR
at FAIR Lars Schmitt, GSI on behalf of the PANDA Collaboration PANIC 2008, Eilat, Israel, November 11th 2008 The Facility Overview of PANDA Physics Summary and Outlook Facility for Antiproton and Ion Research
More informationPhysics with the PANDA Detector at FAIR
II. Physics Institute Justus-Liebig-Universität Giessen, Germany on behalf of the PANDA collaboration SPIN-Praha-2008, July 21 st 2008, Prague PANDA= AntiProton ANnihilations at DArmstadt Physics with
More informationFacility for Antiproton and Ion Research - FAIR
Facility for Antiproton and Ion Research - FAIR Inti Lehmann FAIR Europe EMMI Workshop: 229mTh Nuclear Isomer Clock Overview The FAIR facility The 4 scientific pillars of FAIR Current status Inti Lehmann
More informationExploring dense matter at FAIR: The CBM Experiment
Exploring dense matter at FAIR: The CBM Experiment What s it all about Landmarks of the QCD phase diagram: deconfinement phase transition chiral phase transition critical point 2 Signatures of phase transition
More informationNEW PERSPECTIVES FOR STUDY OF CHARMONIUM AND EXOTICS ABOVE DD THRESHOLD. Barabanov M.Yu., Vodopyanov A.S.
NEW PERSPECTIVES FOR STUDY OF CHARMONIUM AND EXOTICS ABOVE DD THRESHOLD Barabanov M.Yu., Vodopyanov A.S. Veksler-Baldin Laboratory of High Energy Physics Joint Institute for Nuclear Research Dubna, Moscow
More informationLABORATORI NAZIONALI DI FRASCATI SIS-Pubblicazioni
LABORATORI NAZIONALI DI FRASCATI SIS-Pubblicazioni LNF-06/22 (P) 29 August 2006 HADRON PROPERTIES IN THE NUCLEAR MEDIUM THE PANDA PROGRAM WITH pa REACTIONS Olaf N. Hartmann INFN, Laboratori Nazionali di
More informationStars Nuclei Baryons Quarks. STRANGENESS IN NUCLEI UNIQUE OPPORTUNITIES at FAIR Josef Pochodzalla
Stars Nuclei Baryons Quarks STRANGENESS IN NUCLEI UNIQUE OPPORTUNITIES at FAIR Josef Pochodzalla Facility for Antiproton and Ion Research GSI, Darmstadt heavy ion physics nuclear structure atomic and plasma
More informationHadron Spectroscopy Lecture 1 Introduction and Motivation
Hadron Spectroscopy Lecture 1 Introduction and Motivation National Nuclear Physics Summer School at MIT Matthew Shepherd Indiana University Outline 1. Overview and Motivation 1.1.Uniue features of QCD
More informationSpin-physics with Polarized Antiprotons at GSI
http://www.fz-juelich.de/ikp/pax Spin-physics with Polarized Antiprotons at GSI Frank Rathmann Forschungszentrum JülichJ Spin Physics and Beyond, Madison, June 10, 2005 QCD Physics at FAIR (CDR): unpolarized
More informationHigh resolution spectroscopy of hypernuclei with γ-ray detectors
High resolution spectroscopy of hypernuclei with γ-ray detectors multi- hypernuclei H-particle Alessandro Feliciello I.N.F.N. - Sezione di Torino Contents 2 Discovery potential of the strangeness nuclear
More informationM.Yu. Barabanov, A.S. Vodopyanov, A.I. Zinchenko
PERSPECTIVE STUDY OF CHARMONIUM AND EXOTICS IN ANTIPRPOTON-PROTON ANNIHILATION AND PROTON-PROTON COLLSIONS M.Yu. Barabanov, A.S. Vodopyanov, A.I. Zinchenko Joint Institute for Nuclear Research, Joliot-Curie
More informationThe Jefferson Lab 12 GeV Program
The Jefferson Lab 12 GeV Program The Jefferson Lab facilities have undergone a substantial upgrade, both of accelerator, CEBAF, and of the experimental installations. We will discuss the progress to completion
More informationForefront Issues in Meson Spectroscopy
Forefront Issues in Meson Spectroscopy Curtis A. Meyer Carnegie Mellon University 1 Outline of Talk Introduction Meson Spectroscopy Glueballs Expectations Experimental Data Interpretation Hybrid Mesons
More informationINTERNATIONAL SCHOOL OF SUBNUCLEAR PHYSICS
INTERNATIONAL SCHOOL OF SUBNUCLEAR PHYSICS WENNINGER The QGCW Project Quark-Gluon-Colored-World «ETTORE MAJORANA» FOUNDATION AND CENTRE FOR SCIENTIFIC CULTURE INTERNATIONAL SCHOOL OF SUBNUCLEAR PHYSICS
More informationCLEO Results From Υ Decays
CLEO Results From Υ Decays V. Credé 1 2 1 Cornell University, Ithaca, NY 2 now at Florida State University Tallahassee, FL Hadron 05 Outline 1 Introduction The Υ System CLEO III Detector CLEO III Υ Data
More informationMeson spectroscopy at CLAS and CLAS12: the present and the future. Raffaella De Vita INFN Genova for the CLAS Collaboration
Meson spectroscopy at CLAS and CLAS12: the present and the future Raffaella De Vita INFN Genova for the CLAS Collaboration Why hadron spectroscopy? QCD is responsible for most of the visible mass in the
More informationFAIR. Reiner Krücken for the NUSTAR collaboration
NUSTAR @ FAIR Reiner Krücken for the NUSTAR collaboration Physik Department E12 Technische Universität München & Maier-Leibnitz-Laboratory for Nuclear and Particle Physics NUSTAR @ FAIR Nuclear Structure
More informationStatus and Perspectives of Hadron Physics in Europe. Forschungszentrum Jülich in der Helmholtz-Gemeinschaft
Hans Ströher Status and Perspectives of Hadron Physics in Europe Forschungszentrum Jülich in der Helmholtz-Gemeinschaft Europe We are here: Tbilisi (Georgia) Area (EU 15): ~ π x 10 6 km 2 (EU 25): 1.25
More informationM.Yu. Barabanov, A.S. Vodopyanov, A.I. Zinchenko
SRTUDY OF STRONG INTERACTION AND HADRONIC MATTER IN ANTIPROTON-PROTON ANNIHILATION AND PROTON-PROTON COLLISIONS M.Yu. Barabanov, A.S. Vodopyanov, A.I. Zinchenko Joint Institute for Nuclear Research, Joliot-Curie
More informationKai Zhu on behalf of BESIII collaboration Institute of High Energy Physics, Beijing March, Moriond QCD 2015
Kai Zhu on behalf of BESIII collaboration Institute of High Energy Physics, Beijing 21-28 March, Moriond QCD 2015 Introduction Charmonium & Exotics states BESIII experiment and BEPCII Exotic charmonium-like
More informationThe PANDA Experiment. Lars Schmitt, GSI on behalf of the PANDA Collaboration Open PANDA, Mainz, November 19th 2009.
The PANDA Experiment Lars Schmitt, GSI on behalf of the PANDA Collaboration Open Charm @ PANDA, Mainz, November 19th 2009 The Facility Overview of PANDA Physics Summary and Outlook Facility for Antiproton
More informationAn Electron-Nucleon Collider at FAIR
An Electron-Nucleon Collider at FAIR Wolfgang Gradl for the ENC@FAIR study group Institut für Kernphysik Physics at a High Energy Electron Ion Collider Seattle, 19 th October 009 Outline FAIR and PANDA
More informationHigh Energy Frontier Recent Results from the LHC: Heavy Ions I
High Energy Frontier Recent Results from the LHC: Heavy Ions I Ralf Averbeck ExtreMe Matter Institute EMMI and Research Division GSI Helmholtzzentrum für Schwerionenforschung Darmstadt, Germany Winter
More informationCLEO-c: Progress and Future
CLEO-c: Progress and Future David G. Cassel Cornell University Outline Motivations CLEO-c and CESR-c Preliminary CLEO-c Results CLEO-c Gluonic Program Summary and Outlook SURA Washington February 10, 2005
More informationThe Gamma Factory proposal for CERN
The Gamma Factory proposal for CERN Photon-2017 Conference, May 2017 Mieczyslaw Witold Krasny LPNHE, CNRS and University Paris Sorbonne 1 The Gamma Factory in a nutshell Accelerate and store high energy
More informationGeneral Introductory Remarks. gamardshoba. me war germaniidan CGSWHP 04. Forschungszentrum Jülich in der Helmholtz-Gemeinschaft
General Introductory Remarks gamardshoba me mkwia me war germaniidan me wmuschaob Hans Ströher FZ Jülich CGSWHP 04 Forschungszentrum Jülich in der Helmholtz-Gemeinschaft General Introductory Remarks CGSWHP
More informationHeavy Hadron Production and Spectroscopy at ATLAS
Heavy Hadron Production and Spectroscopy at ALAS Carlo Schiavi on behalf of the ALAS Collaboration INFN Sezione di Genova ALAS has studied heavy flavor production and measured the production cross sections
More informationCharmed Baryon spectroscopy at Belle 1. Y. Kato KMI topics. Mainly based on the paper recently accepted by PRD ( arxiv: )
Charmed Baryon spectroscopy at Belle 1 Y. Kato KMI topics Mainly based on the paper recently accepted by PRD ( arxiv:1312.1026) Introduction 2 The mass of matter is almost made of nucleons. But they are
More informationLepton and Charm Measurements in the First Two Years of RHIC: An Experimental Overview
Lepton and Charm Measurements in the First Two Years of RHIC: An Experimental Overview Ralf Averbeck State University of New York at Stony Brook INT/RHIC Winter Workshop, Seattle, December 13-15, 2002
More informationNew Physics Opportunities in the Charm/Tau Region: The BESIII - Experiment at IHEP/Beijing
New Physics Opportunities in the Charm/Tau Region: The BESIII - Experiment at IHEP/Beijing Introduction BES3/BEPC2 Physics Programme First Results Summary 1 W.Kühn, Univ. Giessen Charmonium: Positronium
More informationPart II Particle and Nuclear Physics Examples Sheet 1
T. Potter Lent/Easter Terms 2017 Part II Particle and Nuclear Physics Examples Sheet 1 Matter and Forces 1. (A) Explain the meaning of the terms quark, lepton, hadron, nucleus and boson as used in the
More informationPROBING OF STRONG INTERACTIONS AND HADRONIC MATTER WITH CHARMONIUM-LIKE STUDIES
PROBING OF STRONG INTERACTIONS AND HADRONIC MATTER WITH CHARMONIUM-LIKE STUDIES Mikhail Barabanov, Alexander Vodopyanov (Joint Institute for Nuclear Research, Dubna) in collaboration with Stephen Olsen
More informationPhotoabsorption and Photoproduction on Nuclei in the Resonance Region
Photoabsorption and Photoproduction on Nuclei in the Resonance Region Susan Schadmand Institut für Kernphysik First Workshop on Quark-Hadron Duality Frascati, June 6-8, 2005 electromagnetic probes Hadron
More informationFAIR AT GSI. P. Spiller, GSI, Darmstadt, Germany
FAIR AT GSI P. Spiller, GSI, Darmstadt, Germany Abstract Based on the experience of the existing GSI facility and with the aim to apply new technical concepts in phase space cooling and fast ramping of
More informationCLAS12 at Jefferson Lab
CLAS12 at Jefferson Lab Daria Sokhan University of Glasgow, UK IPPP/NuSTEC Topical Meeting on Neutrino-Nucleus Scattering IPPP, Durham, UK 19 April 2017 Jefferson Lab 6 GeV era Jefferson Lab CEBAF: Continuous
More informationFAIR Facility for Antiproton and Ion Research. Marielle Chartier University of Liverpool
FAIR Facility for Antiproton and Ion Research Marielle Chartier University of Liverpool UK Nuclear Physics Community Meeting, Cosener s House, 25-26 26 May 2005 The Future International Facility at GSI:
More informationThe achievements of the CERN proton antiproton collider
The achievements of the CERN proton antiproton collider Luigi DiLella Scuola Normale Superiore, Pisa, Italy Motivation of the project The proton antiproton collider UA1 and UA2 detectors Discovery of the
More informationDescription of the FAIR facility to be constructed and the stages of construction (Part A) and
November 16, 2009 Technical Document 1 attached to the Convention concerning the construction and operation of a Facility for Antiproton and Ion Research in Europe (FAIR) Description of the FAIR facility
More informationOn Antihyperon-Hyperon Production in Antiproton-Proton Collisions with the PANDA Experiment
On Antihyperon-Hyperon Production in Antiproton-Proton Collisions with the PANDA Experiment A Thesis submitted for the degree of Master of Science in Engineering Physics Catarina E. Sahlberg Department
More informationProbing of XYZ meson structure with near threshold pp and pa collisions
Probing of XYZ meson structure with near threshold pp and pa collisions Mikhail Barabanov, Alexander Vodopyanov, (Joint Institute for Nuclear Research, Dubna) in collaboration with Stephen Olsen (Institute
More informationSimulation studies of the PANDA detector at GSI
Simulation studies of the PANDA detector at GSI Carsten Schwarz for the Antiproton Physics Study Group PANDA = Proton ANtiproton at DArmstadt Introduction HESR (High Energy Storage Ring) Physics program
More informationResults on Charmonium-like States at BaBar
Results on Charmonium-like States at BaBar INFN Ferrara Representing the BaBar Collaboration Outline Introduction and Overview Search for the Z 1 (4050) + and Z 2 (4250) + states in B 0 χ c1 K - π + and
More informationHadron structure with photon and antiproton induced reactions - QCD in the non-perturbative range -
Hadron structure with photon and antiproton induced reactions - QCD in the non-perturbative range - Introduction Present: Photoproduction of Mesons at ELSA and MAMI CB-ELSA/TAPS Experiment Crystal Ball/TAPS
More informationHadron Physics with Real and Virtual Photons at JLab
Hadron Physics with Real and Virtual Photons at JLab Elton S. Smith Jefferson Lab Virtual photons shape of the nucleon Elastic scattering (form factors) Inelastic scattering (uark distributions) Exclusive
More informationThe Jlab 12 GeV Upgrade
The Jlab 12 GeV Upgrade R. D. McKeown Jefferson Lab College of William and Mary 1 12 GeV Science Program The physical origins of quark confinement (GlueX, meson and baryon spectroscopy) The spin and flavor
More informationExecutive Summary. Overview. Section 1
Executive Summary Overview This Conceptual Design Report (CDR) presents the plans for a major new international research facility at the GSI Laboratory (Gesellschaft für Schwerionenforschung) at Darmstadt,
More informationExperimental Program of the Future COMPASS-II Experiment at CERN
Experimental Program of the Future COMPASS-II Experiment at CERN Luís Silva LIP Lisbon lsilva@lip.pt 24 Aug 2012 On behalf of the COMPASS Collaboration co-financed by THE COMPASS EXPERIMENT Common Muon
More informationarxiv: v1 [nucl-ex] 10 Oct 2016
The PANDA Experiment at FAIR - Subatomic Physics with Antiprotons arxiv:1610.02804v1 [nucl-ex] 10 Oct 2016 Johan Messchendorp 1 on behalf of the PANDA Collaboration 1 KVI-CART/University of Groningen,
More informationRecent results on spectroscopy from
Recent results on spectroscopy from LIU Beijiang Institute of High Energy Physics, Beijing (for BESIII collaboration) XVI International Conference on Hadron Spectroscopy, Sept. 13-18, 2015, Newport News,
More informationOverview of the PandaRoot Framework
Overview of the PandaRoot Framework for the Stefano Spataro computing group ISTITUTO NAZIONALE DI FISICA NUCLEARE Sezione di Torino Thuersday, 18th November, 2010 The Panda experiment AntiProton Annihilations
More informationCMS Conference Report
Available on CMS information server CMS CR 2001/004 CMS Conference Report April 13, 2001 Prospects of B-Physics with CMS a) Sunanda Banerjee 1) Abstract Prospects of studies of properties of b flavoured
More informationPhysics with Hadron Beams at COMPASS
Physics with Hadron Beams at COMPASS Bernhard Ketzer Technische Universität München MAMI and Beyond 2009 International Workshop on Hadron Structure and Spectroscopy 2009 30 March 2009 The Goal Understand
More informationStudies of charmonium production in e + e - annihilation and B decays at BaBar
Studies of charmonium production in e + e - annihilation and B decays at BaBar I. Garzia, INFN Sezione di Ferrara On behalf of the BaBar Collaboration XVI International Conference on Hadron Spectroscopy
More informationIn-Kind FAIR. David Urner. FAIR, Darmstadt , D. Urner 1
In-Kind FAIR David Urner FAIR, Darmstadt 4.11.2015, D. Urner 1 Overview Existing Facility HEBT High Energy Beam Transport SIS100 heavy (Schwer) Ion Syncrotron CRYRING HESR High Energy Storage Ring p-bar
More informationThe PANDA experiment: physics goals and experimental setup
PJ Web of Conferences 72, 00002 ( 2014) DOI: 10.1051/ epjconf/ 20147200002 C Owned by the authors, published by DP Sciences, 2014 The PANDA experiment: physics goals and experimental setup Gianluigi Boca,
More informationFAIR. International Facility for Antiproton and Ion. Research
FAIR International Facility for Antiproton and Ion Research FAIR One of the largest scientific project in the world with a broad spectrum of research programs: - Nuclear physics - Hadron physics - Atomic
More informationThe Collider Detector at Fermilab. Amitabh Lath Rutgers University July 25, 2002
The Collider Detector at Fermilab Amitabh Lath Rutgers University July 25, 2002 What is Fermilab? A user facility with the Tevatron: 4 mile ring with superconducting magnets. Collides protons with antiprotons.
More informationLight-Meson Spectroscopy at Jefferson Lab
Light-Meson Spectroscopy at Jefferson Lab Volker Credé Florida State University, Tallahassee, Florida PANDA Collaboration Meeting Uppsala, Sweden 06/10/2015 Outline Introduction 1 Introduction 2 Detector
More informationOverview. The quest of Particle Physics research is to understand the fundamental particles of nature and their interactions.
Overview The quest of Particle Physics research is to understand the fundamental particles of nature and their interactions. Our understanding is about to take a giant leap.. the Large Hadron Collider
More informationGeneralized Partial Wave Analysis Software for PANDA
Generalized Partial Wave Analysis Software for PANDA 39. International Workshop on the Gross Properties of Nuclei and Nuclear Excitations The Structure and Dynamics of Hadrons Hirschegg, January 2011 Klaus
More informationSearch for Gluonic Excitations with GlueX at Jefferson Lab
Search for Gluonic Excitations with GlueX at Jefferson Lab Volker Credé Florida State University Tallahassee, FL The Structure and Dynamics of Hadrons Hirschegg, 01/19/2007 Outline 1 2 3 4 Outline 1 2
More informationMeson Spectroscopy Methods, Measurements & Machines
Meson Spectroscopy Methods, Measurements & Machines Aug. 31 Sep. 4, Groningen Klaus Götzen GSI Darmstadt Mesons are they really interesting? Look at the American Physical Society Highlights 2013! [http://physics.aps.org/articles/v6/139]...
More informationGSI Future Facility. Primary Beams. Secondary Beams. Storage and Cooler Rings. Key Technical Features
P GSI Future Facility SIS 100/300 Primary Beams 10 12 /s; 1.5 GeV/u; 238 U 28+ Factor 100-1000 over present in intensity 2(4)x10 13 /s 30 GeV protons 10 10 /s 238 U 73+ up to 25 (- 35) GeV/u UNILAC 100
More informationSSA Measurements with Primary Beam at J-PARC
SSA Measurements with Primary Beam at J-PARC Joint UNM/RBRC Workshop on Orbital Angular Momentum in Albuquerque February 25 th, 2006 Yuji Goto (RIKEN/RBRC) February 25, 2006 Yuji Goto (RIKEN/RBRC) 2 Introduction
More informationMesons beyond the quark-antiquark picture: glueballs, hybrids, tetraquarks - part 1 - Francesco Giacosa
Mesons beyond the quark-antiquark picture: glueballs, hybrids, tetraquarks - part 1-55 Cracow School of Theoretical Physics 20 28/6/2015, Zakopane, Poland Outline The Lagrangian of QCD and its symmetries
More informationMukesh Saini. Florida State University, Tallahassee, FL. February 26, FSU Nuclear Physics Seminar. February 26
C o l u m n 3 Mukesh Saini Florida State University, Tallahassee, FL, 2010 1 OUTLINE Introduction Meson Spectroscopy Strangeonia Experiment CEBAF & CLAS HyCLAS & g12 Calibrations Analysis Summary 2 QCD
More informationQCD aspects of the antiproton program at GSI
QCD aspects of the antiproton program at GSI H. Koch Ruhr-Universität t Bochum Titel Organizers: Mauro Anselmino, Helmut Koch (Coordinator), Ulrich Mosel, Dan-Olof Riska All talks available: http://www.ep1.ruhr-uni-bochum.de/~dagmar/trento.htm
More informationThe PANDA Experiment
High Precision Hadron Physics at FIR Lars chmitt GI, armstadt First FIR FEE Workshop, October 2005 Outline 1 PN Overview Introduction Physics Program 2 Overview Highlights PN Q and Trigger PN Overview
More informationFuture Prospects for Hadron Physics at PANDA
Ulrich Wiedner Future Prospects for Hadron Physics at PANDA Institut f. Experimentalphysik 1, Ruhr-University Bochum, D-44780 Bochum, Germany Keywords: hadron spectroscopy, charmonium, glueballs and hybrids,
More informationExotic hadronic states XYZ
Exotic hadronic states XYZ Yu-Ping Guo (KPH, Mainz University) International School of Nuclear Physics 37 th Course Probing Hadron Structure with lepton and Hadron Beams Erice-Sicily September 16-4, 15
More informationPaul Reimer showed these two slides at the Jlab User s Group meeting: I have shamelessy copied them.. NNPSS 2009 E. Beise, U Maryland 1
Paul Reimer showed these two slides at the Jlab User s Group meeting: I have shamelessy copied them.. NNPSS 2009 E. Beise, U Maryland 1 NNPSS 2009 E. Beise, U Maryland 2 Hadron Physics Topics I will attempt
More informationNUSTAR and the status of the R3B project at FAIR
PRAMANA c Indian Academy of Sciences journal of physics pp. 1 7 NUSTAR and the status of the R3B project at FAIR 1nstituto de Estructura de la Materia, Consejo Superior de Investigaciones Cientficas, Madrid
More informationRecent Results from the BESIII Experiment. Ryan Mitchell Indiana University Miami 2011 December 17, 2011
Recent Results from the BESIII Experiment Ryan Mitchell Indiana University Miami 11 December 17, 11 1 The primary goal of BESIII: Use e + e collisions to produce charmonium states, then use their properties
More informationHadron Spectroscopy at COMPASS
Hadron Spectroscopy at Overview and Analysis Methods Boris Grube for the Collaboration Physik-Department E18 Technische Universität München, Garching, Germany Future Directions in Spectroscopy Analysis
More informationWeak decay of hypernuclei with FINUDA. Alessandro Feliciello I.N.F.N. - Sezione di Torino
Weak decay of hypernuclei with FINUDA Alessandro Feliciello I.N.F.N. - Sezione di Torino 2 Outlook Introduction The FINUDA experiment Weak decay of hypernuclei mesonic nucleon stimulated rare decay channels
More informationISR physics at BABAR
SLAC-PUB-499 ISR physics at BABAR S.Serednyakov, Budker Institute of Nuclear Physics, Novosibirsk, Russia Abstract A method of measuring e+e- annihilation cross sections at low energy s < 5 GeV, using
More informationThe Super-FRS Project at GSI
2 m A G A T A The Super-FRS Project at GSI FRS facility The concept of the new facility The Super-FRS and its branches Summary Martin Winkler for the Super-FRS working group CERN, 3.1.22 Energy Buncher
More information(a) (b) Fig. 1 - The LEP/LHC tunnel map and (b) the CERN accelerator system.
Introduction One of the main events in the field of particle physics at the beginning of the next century will be the construction of the Large Hadron Collider (LHC). This machine will be installed into
More information