PaperPanorama

Nuclear Theory·nucl-th

Tuesday·March 14, 2017

8 papers5 primary·3 cross-listed

  1. 06

    Valence quark contributions for the form factors from Light-Front holography

    G. Ramalho🇧🇷 · D. Melnikov🇧🇷

    The structure of the nucleon and the first radial excitation of the nucleon, the Roper, , is studied within the formalism of Light-Front holography. The nucleon elastic form factors and transition form factors are calculated under the assumption of the dominance of the valence quark degrees of freedom. Contrary to the previous studies, the bare parameters of the model associated with the valence quark are fixed by the empirical data for large momentum transfer () assuming that the corrections to the three-quark picture (meson cloud contributions) are suppressed. The transition form factors are then calculated without any adjustable parameters. Our estimates are compared with results from models based on valence quarks and others. The model compares well with the transition form factor data, suggesting that meson cloud effects are not large, except in the region GeV. In particular, the meson cloud contributions for the Pauli form factor are small.

    hep-phhep-exnucl-exnucl-thPRD(2018)·28 citations
  2. 07

    Topology and stability of the Kondo phase in quark matter

    Shigehiro Yasui🇯🇵 · Kei Suzuki🇯🇵 · Kazunori Itakura🇯🇵

    We investigate properties of the ground state of a light quark matter with heavy quark impurities. This system exhibits the "QCD Kondo effect" where the interaction strength between a light quark near the Fermi surface and a heavy quark increases with decreasing energy of the light quark towards the Fermi energy, and diverges at some scale near the Fermi energy, called the Kondo scale. Around and below the Kondo scale, we must treat the dynamics nonperturbatively. As a typical nonperturbative method to treat the strong coupling regime, we adopt a mean-field approach where we introduce a condensate, the Kondo condensate, representing a mixing between a light quark and a heavy quark, and determine the ground state in the presence of the Kondo condensate. We show that the ground state is a topologically non-trivial state and the heavy quark spin forms the hedgehog configuration in the momentum space. We can define the Berry phase for the ground-state wavefunction in the momentum space which is associated with a monopole at the position of a heavy quark. We also investigate fluctuations around the mean field in the random-phase approximation, and show the existence of (exciton-like) collective excitations made of a hole of a light quark and a heavy quark .

    hep-phcond-mat.str-elnucl-thPRD(2017)·22 citations
  3. 08

    Quark spin polarization and spontaneous magnetization in high density quark matter

    Y. Tsue (Kochi Univ., Japan)🇯🇵 · J. da Providencia (Univ. de Coimbra, Portugal)🇵🇹 · C. Providencia (Univ. de Coimbra, Portugal)🇵🇹 · H. Matsuoka (Kochi Univ., Japan)🇯🇵 · M. Yamamura (Kansai Univ., Japan)🇯🇵 · H. Bohr (Danish Technical Univ., Denmark)🇩🇰

    By using the Nambu-Jona-Lasinio model with a tensor-type four-point interaction between quarks, it is shown that there exists a possibility of a spin polarized phase in quark matter at finite temperature and density. When there exists the spin polarization, the spontaneous magnetization may occur if the effect of the anomalous magnetic moment of quark is taken into account. An implication to the compact star objects with strong magnetic field is discussed when the spin polarization occurs.

    hep-phnucl-thPoS(2017)·0 citations

Affiliations

first authorsco-authorsvia INSPIRE