VALENCIA, Julio 2014. Pedro González THE THREE QUARK FRENCH CONNECTION.

Slides:



Advertisements
Similar presentations
1 Eta production Resonances, meson couplings Humberto Garcilazo, IPN Mexico Dan-Olof Riska, Helsinki … exotic hadronic matter?
Advertisements

Excited Charm and K0sK0s Resonance Production at ZEUS V. Aushev For the ZEUS Collaboration XXXIX International Symposium on Multiparticle Dynamics ''Gold.
Dynamical Anisotropic-Clover Lattice Production for Hadronic Physics C. Morningstar, CMU K. Orginos, College W&M J. Dudek, R. Edwards, B. Joo, D. Richards,
Recent development of the Constituent Quark Model including quark-antiquark effects and confinement. E. Santopinto and R. Bijker Dedicated to Nathan Isgur.
NSTAR 2007Roelof Bijker, ICN-UNAM1 Flavor Asymmetry of the Nucleon Sea in an Unquenched Quark Model Introduction Degrees of freedom Unquenched quark model.
Symmetries By Dong Xue Physics & Astronomy University of South Carolina.
Functional renormalization – concepts and prospects.
Chiral freedom and the scale of weak interactions.
QCD – from the vacuum to high temperature an analytical approach an analytical approach.
Table of contents 1. Motivation 2. Formalism (3-body equation) 3. Results (KNN resonance state) 4. Summary Table of contents 1. Motivation 2. Formalism.
University of Birmingham Master class,23rd April 2008 Ravjeet Kour Journey into the heart of matter Introducing Particle Physics.
Chiral freedom and the scale of weak interactions.
Qiang Zhao Institute of High Energy Physics, CAS, P.R. China Department of Physics, University of Surrey, U.K. Baryons in a potential quark model Selection.
Scalar  and  interaction within a chiral unitary approach HYP2006, Mainz,13 th Oct 2006 Kenji Sasaki E. Oset M. J. Vicente Vacas (Valencia University.
Nuclear and Radiation Physics, BAU, First Semester, (Saed Dababneh). 1 Nuclear Force Spin dependent  difference in neutron scattering cross.
Lecture 10: Inelastic Scattering from the Proton 7/10/2003
Ralf W. Gothe Nucleon Transition Form Factors Beijing Transition Form Factors at JLab: The Evolution of Baryonic Degrees of Freedom Ralf W. Gothe.
Highlights on hadron physics at CLAS K. Hicks JAEA Seminar May 18, 2012.
Generalities of the approaches for extraction of N* electrocouplings at high Q 2 Modeling of resonant / non resonant contributions is needed and should.
Toshitaka Uchino Tetsuo Hyodo, Makoto Oka Tokyo Institute of Technology 10 DEC 2010.
Sigma model and applications 1. The linear sigma model (& NJL model) 2. Chiral perturbation 3. Applications.
Tension Between A Fourth Generation And The LHC Higgs Searches Xiao-Gang He (SJTU&NTU) Xiao-Gang He and German Valencia, arXiv: Xiao-Gang He and.
Chapters 9, 11, 12 Concepts covered that will also be candidates for exam questions.
Kab/SC-PAC Operated by the Jefferson Science Associates for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility SURA.
The Baryon octet-vector meson interaction and dynamically generated resonances in the S=0 sector Bao-Xi SUN ( 孙宝玺 ) Beijing University of Technology Hirschegg.
PATTERNS IN THE NONSTRANGE BARYON SPECTRUM P. González, J. Vijande, A. Valcarce, H. Garcilazo.
Chiral Symmetry Restoration and Deconfinement in QCD at Finite Temperature M. Loewe Pontificia Universidad Católica de Chile Montpellier, July 2012.
Munich, June 16th, 2010Exotic gifts of nature1 XIV International Conference on Hadron Spectroscopy J. Vijande University of Valencia (Spain) A. Valcarce,
Molecular Charmonium. A new Spectroscopy? II Russian-Spanish Congress Particle and Nuclear Physics at all Scales and Cosmology F. Fernandez D.R. Entem,
Probe resolution (GeV) N π,  Q 2 =12 GeV 2 Q 2 =6 GeV 2 The study of nucleon resonance transitions provides a testing ground for our understanding.
N* Production in α-p and p-p Scattering (Study of the Breathing Mode of the Nucleon) Investigation of the Scalar Structure of baryons (related to strong.
Chiral phase transition and chemical freeze out Chiral phase transition and chemical freeze out.
Particles and how they interact
Hadron Spectroscopy with high momentum beam line at J-PARC K. Ozawa (KEK) Contents Charmed baryon spectroscopy New experiment at J-PARC.
Measurement of high lying nucleon resonances and search for missing state in double charged pion electroproduction off proton E.Golovach for the CLAS collaboration.
Nov. 12, HAPHY. A QCD sum rule analysis of the PLB 594 (2004) 87, PLB 610 (2005) 50, and hep-ph/ Hee-Jung Lee Vicente Vento (APCTP & U. Valencia)
Multiplet Structure - Isospin and Hypercharges. As far as strong interactions are concerned, the neutron and the proton are the two states of equal mass.
Nucleon and Roper on the Lattice Y. Chen Institute of High Energy Physics, CAS, China Collaborating with S.J. Dong, T. Draper, I. Horvath, F.X. Lee, K.F.
Chiral symmetry breaking and low energy effective nuclear Lagrangian Eduardo A. Coello Perez.
R. Machleidt, University of Idaho Recent advances in the theory of nuclear forces and its relevance for the microscopic approach to dense matter.
Time Dependent Quark Masses and Big Bang Nucleosynthesis Myung-Ki Cheoun, G. Mathews, T. Kajino, M. Kusagabe Soongsil University, Korea Asian Pacific Few.
1 Longitudinal and transverse helicity amplitudes of nucleon resonances in a constituent quark model - bare vs dressed resonance couplings Introduction.
PLAUSIBLE EXPLANATION FOR THE   (2000) PUZZLE HADRON 2011 XIV International Conference On Hadron Spectroscopy München, June 2011.
Study of e+e- annihilation at low energies Vladimir Druzhinin Budker Institute of Nuclear Physics (Novosibirsk, Russia) SND - BaBar Lepton-Photon, August,
XXXI Bienal de la RSEF, Granada, España, septiembre Angel Gómez Nicola Universidad Complutense Madrid COEFICIENTES DE TRANSPORTE EN UN GAS.
Exotic baryon resonances in the chiral dynamics Tetsuo Hyodo a a RCNP, Osaka b ECT* c IFIC, Valencia d Barcelona Univ. 2003, December 9th A.Hosaka a, D.
THE PREDICTION OF LEPTONIC DECAY WIDTHS IN THE FRAME WORK OF CONSTITUENT QUARK MODELS BY DR. K.B. VIJAYA KUMAR READER,DEPARTMENT OF PHYSICS MANGALORE UNIVERSITY.
Low energy reaction K - p → Λη and the negative parity Λ resonances Liye Xiao (肖立叶) tutor: Xianhui Zhong The Seventh International Symposium on Chiral.
Pentaquark decay width in QCD sum rules F.S. Navarra, M. Nielsen and R.R da Silva University of São Paulo, USP Brazil (  decay width) hep-ph/ (
ANALYTIC APPROACH TO CONSTRUCTING EFFECTIVE THEORY OF STRONG INTERACTIONS AND ITS APPLICATION TO PION-NUCLEON SCATTERING A.N.Safronov Institute of Nuclear.
Possible molecular bound state of two charmed baryons - hadronic molecular state of two Λ c s - Wakafumi Meguro, Yan-Rui Liu, Makoto Oka (Tokyo Institute.
1 Keitaro Nagata and Atsushi Hosaka Research Center for Nuclear Physics, Osaka Univ. Quark-Diquark approach for the nucleon and Roper resonance Workshop.
Hadron 2015 / A. Valcarce1/19 Unraveling the pattern of XYZ mesons. Phys. Lett. B 736, 325 (2014) Phys. Rev. Lett. 103, (2009); Phys. Rev. D 79,
Beijing, QNP091 Matthias F.M. Lutz (GSI) and Madeleine Soyeur (Saclay) Irfu/SPhN CEA/ Saclay Irfu/SPhN CEA/ Saclay Dynamics of strong and radiative decays.
Hadron 2007 Frascati, October 12 th, 2007 P.Faccioli, M.Cristoforetti, M.C.Traini Trento University & I.N.F.N. J. W. Negele M.I.T. P.Faccioli, M.Cristoforetti,
Meson and Baryon Resonances from the interaction of vector mesons Hidden gauge formalism for vector mesons, pseudoscalars and photons Derivation of chiral.
CHARM th International Workshop on Charm Physics Honolulu May
University of Salamanca
Baryons on the Lattice Robert Edwards Jefferson Lab Hadron 09
Institute of High Energy physics KEK, Hadron physics at J-PARC, Japan
mesons as probes to explore the chiral symmetry in nuclear matter
Lecture 04 - Hadrons Quarks multiplets Hadron decays Resonances
Relativistic Chiral Mean Field Model for Finite Nuclei
Exotic charmed four-quark mesons: molecules versus compact states
Spontaneous P-parity breaking in QCD at large chemical potentials
Charm2010 4TH International Workshop on Charm Physics
Charmonium spectroscopy above thresholds
HADRON 2015 XVI International Conference on Hadron Spectroscopy
AN EXPLANATION OF THE D5/2-(1930) AS A rD BOUND STATE
Physics 4 – April 18, 2019 Agenda:
Presentation transcript:

VALENCIA, Julio 2014

Pedro González THE THREE QUARK FRENCH CONNECTION

Inversion Problem in Baryon Spectroscopy In quark models based on reasonable two-quark interactions (OGE, OBE) the first excited state of negative parity lies in general below the first excitation of positive parity. Is it possible to implement an effective quark interaction to solve this problem?

BCN two-quark InteractionBertrand’s three-quark Interaction

What may be representing this effective potential? The effect of genuine three-quark forces (two sigma exchange) A way to take into account other corrections (relativistic, chiral, meson-baryon components…)

In order to really check the validity of a quark model to explain the baryon structure one has to go beyond the description of the spectral masses and consider transition processes. EEM3P0

STRONG PION DECAY WIDTHS Conclusion: Meson-baryon components implemented through the 3P0 model play a very relevant role in the description of the first positive parity excitations. Roper resonances have significant 3q as well as meson-baryon components. EEM3P0 EXP

VALENCIA, Julio 2014