PaperPanorama

Nuclear Theory·nucl-th

Wednesday·January 13, 2016

8 papers5 primary·3 cross-listed

  1. 06

    The hidden-charm pentaquark and tetraquark states

    Hua-Xing Chen🇨🇳 · Wei Chen🇨🇦 · Xiang Liu🇨🇳 · Shi-Lin Zhu🇨🇳

    In the past decade many charmonium-like states were observed experimentally. Especially those charged charmonium-like states and bottomonium-like states can not be accommodated within the naive quark model. These charged states are good candidates of either the hidden-charm tetraquark states or molecules composed of a pair of charmed mesons. Recently, the LHCb Collaboration discovered two hidden-charm pentaquark states, which are also beyond the quark model. In this work, we review the current experimental progress and investigate various theoretical interpretations of these candidates of the multiquark states. We list the puzzles and theoretical challenges of these models when confronted with the experimental data. We also discuss possible future measurements which may distinguish the theoretical schemes on the underlying structures of the hidden-charm multiquark states.

    hep-phhep-exhep-latnucl-ex+1Phys.Rept.(2016)·1460 citations
  2. 07

    Holographic Nambu Jona-Lasinio Interactions

    Nick Evans🇬🇧 · Keun-Young Kim🇰🇷

    NJL interactions are introduced into the D3/ probe D7 system using Witten's double trace operator prescription which includes the operator as a classical term in the effective potential. In the supersymmetric system they do not induce chiral symmetry breaking which we attribute to the flat effective potential with quark mass in the supersymmetric theory. If additional supersymmetry breaking is introduced then standard NJL behaviour is realized. In examples where chiral symmetry breaking is not preferred such as with a B field plus an IR cut off chiral condensation is triggered by the NJL interaction at a second order transition after a finite critical coupling. If the model already contains chiral symmetry breaking, for example in the B field case with no IR cut off, then the NJL interaction enhances the quark mass at all values of the NJL coupling. We also consider the system at finite temperature: the temperature discourages condensation but when combined with a magnetic field we find regions of parameter space where the NJL interaction triggers a first order chiral transition above a critical coupling.

    hep-thnucl-thPRD(2016)·18 citations
  3. 08

    Nuclear collisions at the Future Circular Collider

    N. Armesto🇪🇸 · A. Dainese🇮🇹 · D. d'Enterria🇨🇭 · S. Masciocchi🇩🇪 · C. Roland🇺🇸 · C.A. Salgado🇪🇸 · M. van Leeuwen🇳🇱 · U.A. Wiedemann🇨🇭

    The Future Circular Collider is a new proposed collider at CERN with centre-of-mass energies around 100 TeV in the pp mode. Ongoing studies aim at assessing its physics potential and technical feasibility. Here we focus on updates in physics opportunities accessible in pA and AA collisions not covered in previous Quark Matter contributions, including Quark-Gluon Plasma and gluon saturation studies, novel hard probes of QCD matter, and photon-induced collisions.

    hep-phhep-exnucl-exnucl-thNPA(2016)·10 citations

Affiliations

first authorsco-authorsvia INSPIRE