Structure of Matter. Nucleons and quarks 1950’s: nucleons are not elementary 1960++: quark model and QCD (Nobel prize 2004) 2007++: Higgs particle discovered?

Slides:



Advertisements
Similar presentations
Introduction. November 2002 Good News House Senate.
Advertisements

Günther Rosner EUROHORC/NuPECC, Paris, 29/11/04 1 Hadron Structure & Spectroscopy Experimental frontiers: High precision High intensity Theoretical symbiosis:
Hadron Physics with Antiprotons – the PANDA Program Olaf N. Hartmann GSI Darmstadt, Germany INPC 2004 · Göteborg, Sweden.
Guenther Rosner FAIR - UK DL, 11/10/06 1 Collaboration Universität Basel, IHEP Beijing, [University of Birmingham] Ruhr- Universität Bochum,
Introduction Glasgow’s NPE research Group uses high precision electromagnetic probes to study the subatomic structure of matter. Alongside this we are.
The Physics of Nuclei, Nuclear Matter and Nucleosynthesis Report of the Nuclear Physics Advisory Panel.
Hierarchies of Matter matter crystal atom atomic nucleus nucleon quarks m m m m < m (macroscopic) confinement hadron.
1. The Physics Case 2. Present Status 3. Hypersystems in pp Interactions 4. The Experiment Future Experiments on Hypernuclei and Hyperatoms _.
Application of Straw Tube Detectors to Hyperon Studies Sedigheh Jowzaee Symposium on Applied Nuclear Physics and Innovative Technologies Sep. 2014,
HL- May 2, 2006Kernfysica: quarks, nucleonen en kernen1 Nuclear Physics: quarks, nucleons and nuclei (QNK) Prof. dr. G. van der Steenhoven and Prof. dr.
Particle Physics and LHC Physics David Krofcheck Canterbury Teachers Workshop July 18 th D. KrofcheckCanterbury Teachers Workshop1.
Concept of the PANDA Detector for pp&pA at GSI Physical motivation for hadron physics with pbars The antiproton facility Detector concept Selected simulation.
Chiral dynamics in hard processes M.V.Polyakovhttp:// Ruhr-University Bochum  Chiral symmetry breaking - the phenomenon shaping.
New Opportunities for Hadron Physics with the Planned PANDA Detector
Centauro and STrange Object Research (CASTOR) - A specialized detector system dedicated to the search for Centauros and Strangelets in the baryon dense,
Outlook towards future Polish participation in the new Accelerator Facility Tomasz Matulewicz Warsaw University.
Spectroscopy of Heavy Quarkonia Holger Stöck University of Florida Representing the CLEO Collaboration 6 th International Conference on Hyperons, Charm.
Polish-German Meeting, Warszawa, Search for exotic hadrons with the PANDA detector Jan Kisiel Institute of Physics, University of Silesia Katowice,
Department of Physics and Astronomy
James Ritman Univ. Giessen PANDA: Experiments to Study the Properties of Charm in Dense Hadronic Matter Overview of the PANDA Pbar-A Program The Pbar Facility.
Hadron Physics with polarized photons at 9 GeV with GlueX Richard Jones University of Connecticut UConn Physics Graduate Studies Open House, Mar. 19, 2010.
TIME-LIKE BARYON FORM FACTORS: EXPERIMENTAL SITUATION AND POSSIBILITIES FOR PEP-N Roberto Calabrese Dipartimento di Fisica and I.N.F.N. Ferrara, Italy.
The CMS Muon Detector Thomas Hebbeker Aachen July 2001 Searching for New Physics with High Energy Muons.
Fundamental Particles (The Standard Model) Nathan Brown June 2007.
Experiment HUGS 2011 – Jefferson Laboratory Hussein Al Ghoul Department Of Physics Florida State University ᵠ.
Working Group 5 Summary David Christian Fermilab.
Spectroscopy: Experimental Status and Prospects Curtis A. Meyer Carnegie Mellon University.
Future Opportunities at an Electron-Ion Collider Oleg Eyser Brookhaven National Laboratory.
Meson spectroscopy with photo- and electro-production Curtis A. Meyer Carnegie Mellon University.
Antiproton Physics at GSI Introduction The antiproton facility The physics program - Charmonium spectroscopy - Hybrids and glueballs - Interaction of charm.
Finishing things up. So what’s with that 14 C? Masses of isotopes (not “natural” stuff) truly are multiples of basic hydrogen. Hydrogen is positively.
Particle Physics Quiz EPPOG Hands on Particle Physics Masterclasses 2011.
1 Plans for JINR participation at FAIR JINR Contributions: ● Accelerator Complex ● Condensed Baryonic Matter ● Antiproton Physics ● Spin Physics Physics.
First Results of Curtis A. Meyer GlueX Spokesperson.
Hadron physics Hadron physics Challenges and Achievements Mikhail Bashkanov University of Edinburgh UK Nuclear Physics Summer School I.
Sub-Nucleon Physics Programme Current Status & Outlook for Hadron Physics D G Ireland.
General Discussion some general remarks some questions.
Relativistic Heavy Ion Collider and Ultra-Dense Matter.
Hadron Spectroscopy with high momentum beam line at J-PARC K. Ozawa (KEK) Contents Charmed baryon spectroscopy New experiment at J-PARC.
22 September 2005 Haw05 1  (1405) photoproduction at SPring-8/LEPS H. Fujimura, Kyoto University Kyoto University, Japan K. Imai, M. Niiyama Research.
James Ritman Univ. Giessen PANDA: An Experiment To Investigate Hadron Structure Using Antiproton Beams Overview of the GSI Upgrade Overview of the PANDA.
Günther Rosner EINN05, Milos, 24/9/05 1 Prospects for Hadron Physics in Europe Experimental frontiers:  High precision  High luminosity  Polarisation.
Introduction to CERN Activities
1 Methods of Experimental Particle Physics Alexei Safonov Lecture #15.
CEBAF - Continuous Electron Beam Accelerator Facility.
Goals of future p-pbar experiment Elmaddin Guliyev Student Seminar, KVI, Groningen University 6 November 2008.
Exploring QCD with Antiprotons PANDA at FAIR M. Hoek on behalf of the PANDA Collaboration IOP Nuclear and Particle Physics Divisional Conference 4-7 April.
SYNTHESIS The Standard Model 1.Elementary particles 2.Strong nuclear force 3.Weak nuclear force 4.The Standard Model.
1 LHCb CMS ALICE ATLAS The ATLAS experiment at the LHC 27 km.
Günther Rosner FAIR UK DL, 25/01/06 1 antiProton Annihilation at DArmstadt Physics programme  Quark confinement: Charmonium spectroscopy 
Inti Lehmann Facility for Antiproton and Ion Research Darmstadt, Germany 2nd PhD Science GSI 2014 – 11 August 2014 FAIR – Facility for Antiproton.
Marc Vanderhaeghen 1 Introduction LEPP16 Marc Vanderhaeghen LEPP16 Workshop Kupferberg, Mainz, April 4-7, 2016 New Vistas in Low-Energy Precision Physics.
PANDA experiment at FAIR (JINR Participation) project PANDA A.G.Olshevskiy for JINR PANDA team VBLHEP – DLNP – LIT - BLTP.
Standard Model of Particle Physics
Exotics as a Probe of Confinement
Nuclear Physics -- Today and Tomorrow From the infinitely strong –
Gluonic Hadrons: A Probe of Confinement
Masses, Forces, Higgs and Gluons
Plans for nucleon structure studies at PANDA
Samples of Hall B Results with Strong Italian Impact
Physics Opportunities with heavy quark system at FAIR
Particle Physics Theory
History of Particle Nuclear Physics!
Particle physics at the LHC and ATLAS.
CMS Masterclass 2017.
how is the mass of the nucleon generated?
CMU Undergraduate Colloquium
Physics 4 – April 18, 2019 Agenda:
Determination of the gluon polarisation
u c s b d n Hadron & Nuclear Physics Particle Physics Quarks Leptons
Presentation transcript:

Structure of Matter

Nucleons and quarks 1950’s: nucleons are not elementary : quark model and QCD (Nobel prize 2004) : Higgs particle discovered? (at LHC) have we understood the strong interaction?

How is the mass created? What is the role of quarks and gluons? Only few % of the hadronic mass can be explained by the Higgs Mechanism! No!!! There might be Experimental surprises! (flux tube animation by D. Leinweber et al.) Do other than 2, 3 quark objects exist?

Some Places to Explore Non-Pertubative QCD charmonium spectroscopy gluonic excitations (hybrids, glueballs)  -ray spectroscopy of hypernuclei

Charmonium Spectroscopy narrow states! many states and transitions not understood!! positronium of QCD! transition region between two limits: massless and heavy-quark!

hybrids: “ordinary” quark states containing excited glue Gluonic Excitations glueballs: gluonic states without valence quark contribution

Stranges s Neutron Number Extension of the Nuclear Chart We do not yet understand the interaction of normal matter with hyperon matter!

The PANDA experiment site within FAIR

beam interaction point solenoid dipole EM and hadron calorimeters target generator RICH drift or wire chambers TOF stop hypernuclei target and detectors muon counters 2m