PaperPanorama

Nuclear Theory·nucl-th

Friday·January 9, 2015

4 papers2 primary·2 cross-listed

  1. 03

    Constraining the density dependence of the nuclear symmetry energy from an X-ray bursting neutron star

    Hajime Sotani🇯🇵 · Kei Iida🇯🇵 · Kazuhiro Oyamatsu🇯🇵

    Neutrons stars lighter than the Sun are basically composed of nuclear matter of density up to around twice normal nuclear density. In our recent analyses, we showed that possible simultaneous observations of masses and radii of such neutron stars could constrain , a combination of the incompressibility of symmetric nuclear matter and the density derivative of the nuclear symmetry energy that characterizes the theoretical mass-radius relation. In this paper, we focus on the mass-radius constraint of the X-ray burster 4U 1724-307 given by Suleimanov et al. (2011). We therefrom obtain the constraint that should be larger than around 130 MeV, which in turn leads to larger than around 110, 98, 89, and 78 MeV for , 230, 280, and 360 MeV. Such a constraint on is more or less consistent with that obtained from the frequencies of quasi-periodic oscillations in giant flares observed in soft-gamma repeaters.

    astro-ph.HEnucl-thPRC(2015)·18 citations
  2. 04

    Graphene as a Lattice Field Theory

    Simon Hands🇬🇧 · Wes Armour🇬🇧 · Costas Strouthos🇨🇾

    We introduce effective field theories for the electronic properties of graphene in terms of relativistic fermions propagating in 2+1 dimensions, and outline how strong inter-electron interactions may be modelled by numerical simulation of a lattice field theory. For strong enough coupling an insulating state can form via condensation of particle-hole pairs, and it is demonstrated that this is a theoretical possibility for monolayer graphene. For bilayer graphene the effect of an interlayer bias voltage can be modelled by the introduction of a chemical potential (akin to isopsin chemical potential in QCD) with no accompanying sign problem; simulations reveal the presence of strong interactions among the residual degrees of freedom at the resulting Fermi surface, which is disrupted by an excitonic condensate. We also present preliminary results for the quasiparticle dispersion, which permit direct estimates of both the Fermi momentum and the induced gap.

    cond-mat.str-elhep-latnucl-thPoS(2015)·2 citations

Affiliations

first authorsco-authorsvia INSPIRE