PaperPanorama

Nuclear Theory·nucl-th

Monday·May 29, 2017

5 papers2 primary·3 cross-listed

  1. 01

    Pairing properties from random distributions of single-particle energy levels

    A. A. Mamun · C. Constantinou · M. Prakash

    Exploiting the similarity between the bunched single-particle energy levels of nuclei and of random distributions around the Fermi surface, pairing properties of the latter are calculated to establish statistically-based bounds on the basic characteristics of the pairing phenomenon. When the most probable values for the pairing gaps germane to the BCS formalism are used to calculate thermodynamic quantities, we find that while the ratio of the critical temperature Tc to the zero-temperature pairing gap is close to its BCS Fermi gas value, the ratio of the superfluid to the normal phase specific heats at Tc differs significantly from its Fermi gas counterpart. The largest deviations occur when a few levels lie closely on either side of the Fermi energy but other levels are far away from it. The influence of thermal fluctuations, expected to be large for systems of finite number of particles, were also investigated using a semiclassical treatment of fluctuations. When the average pairing gaps along with those differing by one standard deviations are used, the characteristic discontinuity of the specific heat at Tc in the BCS formalism was transformed to a shoulder-like structure indicating the suppression of a second order phase transition as experimentally observed in nano-particles and several nuclei. Contrasting semiclassical and quantum treatments of fluctuations for the random spacing model is currently underway.

    nucl-thPRC(2018)·2 citations
  2. 02

    SU(4) flavor symmetry breaking in D-meson couplings to light hadrons

    C.E. Fontoura🇧🇷 · J. Haidenbauer🇩🇪 · G. Krein🇧🇷

    The validity of SU(4)-flavor symmetry relations of couplings of charmed mesons to light mesons and baryons is examined with the use of quark-pair creation model and nonrelativistic quark model wave functions. We focus on the three-meson couplings , and and baryon-baryon-meson couplings , and . It is found that SU(4)-flavor symmetry is broken at the level of 30% in the tree-meson couplings and 20% in the baryon-baryon-meson couplings. Consequences of these findings for DN cross sections and existence of bound states D-mesons in nuclei are discussed.

    nucl-thhep-phEPJA(2017)·16 citations
  3. 03

    Fermions in Two Dimensions: Scattering and Many-Body Properties

    Alexander Galea · Tash Zielinski · Stefano Gandolfi · Alexandros Gezerlis

    Ultracold atomic Fermi gases in two-dimensions (2D) are an increasingly popular topic of research. The interaction strength between spin-up and spin-down particles in two-component Fermi gases can be tuned in experiments, allowing for a strongly interacting regime where the gas properties are yet to be fully understood. We have probed this regime for 2D Fermi gases by performing T=0 ab initio diffusion Monte Carlo calculations. The many-body dynamics are largely dependent on the two-body interactions, therefore we start with an in-depth look at scattering theory in 2D. We show the partial-wave expansion and its relation to the scattering length and effective range. Then we discuss our numerical methods for determining these scattering parameters. We close out this discussion by illustrating the details of bound states in 2D. Transitioning to the many-body system, we use variationally optimized wave functions to calculate ground-state properties of the gas over a range of interaction strengths. We show results for the energy per particle and parametrize an equation of state. We then proceed to determine the chemical potential for the strongly interacting gas.

    cond-mat.quant-gasnucl-thJ.Low Temp.Phys.(2017)·5 citations
  4. 04

    Chiral magnetohydrodynamics for heavy-ion collisions

    Yuji Hirono🇺🇸

    The chiral magnetic effect (CME) is a macroscopic transport effect resulting from the chiral anomaly. We review the recent progress in theoretical understanding the properties of chiral plasmas, in which the CME and other anomaly-induced transports take place. In particular, the nontrivial interplay of anomalous currents and dynamical electromagnetic fields is discussed. We also review the theoretical status of the modeling of anomalous transport effects in heavy-ion collisions.

    hep-phnucl-thNPA(2017)·5 citations
  5. 05

    Comment on "On the implementation of CVC in weak charged-current proton-neutron transitions" by C. Giunti, arXiv: 1602.00215 [hep-ph]

    A. N. Ivanov🇦🇹

    We show that the term maintaining conservation of the charged vector current for the transitions "neutron <-> proton" even for different masses of the neutron and proton (see T. Leitner et al., Phys. Rev. C {\bf 73}, 065502 (2006) and A. M. Ankowski, arXiv:1601.06169 [hep-ph]) is related to the first class current contribution but not to the second class one as has been pointed out by C. Giunti, arXiv: 1602.00215 [hep-ph].

    hep-phastro-ph.COhep-exnucl-ex+15 citations

Affiliations

first authorsco-authorsvia INSPIRE