PaperPanorama

Nuclear Theory·nucl-th

Thursday·April 19, 2018

6 papers5 primary·1 cross-listed

  1. 01

    Bayesian parameter estimation for relativistic heavy-ion collisions

    Jonah E. Bernhard🇺🇸

    I develop and apply a Bayesian method for quantitatively estimating properties of the quark-gluon plasma (QGP), an extremely hot and dense state of fluid-like matter created in relativistic heavy-ion collisions. The QGP cannot be directly observed -- it is extraordinarily tiny and ephemeral, about meters in size and living seconds before freezing into discrete particles -- but it can be indirectly characterized by matching the output of a computational collision model to experimental observations. The model, which takes the QGP properties of interest as input parameters, is calibrated to fit the experimental data, thereby extracting a posterior probability distribution for the parameters. In this dissertation, I construct a specific computational model of heavy-ion collisions and formulate the Bayesian parameter estimation method, which is based on general statistical techniques. I then apply these tools to estimate fundamental QGP properties, including its key transport coefficients and characteristics of the initial state of heavy-ion collisions. Perhaps most notably, I report the most precise estimate to date of the temperature-dependent specific shear viscosity , the measurement of which is a primary goal of heavy-ion physics. The estimated minimum value is (posterior median and 90% uncertainty), remarkably close to the conjectured lower bound of . The analysis also shows that likely increases slowly as a function of temperature. Other estimated quantities include the temperature-dependent bulk viscosity , the scaling of initial state entropy deposition, and the duration of the pre-equilibrium stage that precedes QGP formation.

    nucl-thhep-phnucl-exstat.AP106 citations
  2. 02

    Coulomb Energy of alpha-Aggregates on a Soap Bubble Shape

    Akihiro Tohsaki · Naoyuki Itagaki

    We study the property of alpha-aggregates on a soap bubble shape within a microscopic framework, which takes full account of the Pauli principle. Our special attention is payed to the Coulomb energy for such an exotic shapes of nuclei, and we discuss the advantage of alpha-clusters with geometric configurations compared with the uniform density distributions in reducing the repulsive effect. We consider four kinds of configurations of alpha clusters on a soap bubble, which are dual polyhedra composed of a dodecahedron and an icosahedron, octacontahedron and two types of truncated icosahedrons, that is, two kinds of Archimedean solids. The latter two are an icosidodecahedron and a fullerene shape. When putting each alpha-cluster on the vertex of polyhedra, four -cluster aggregates correspond to the following four nuclei; Gd (64 protons), Po (84 protons), Nd (60 protons) and a nucleus with 120 protons, respectively.

    nucl-thPRC(2018)·4 citations
  3. 03

    Disappearance of nuclear deformation in hypernuclei: a perspective from a beyond-mean-field study

    H. Mei · K. Hagino · J.M. Yao · T. Motoba

    The previous mean-field calculation [Myaing Thi Win and K. Hagino, Phys. Rev. C{\bf 78}, 054311 (2008)] has shown that the oblate deformation in Si disappears when a particle is added to these nuclei. We here investigate this phenomenon by taking into account the effects beyond the mean-field approximation. To this end, we employ the microscopic particle-rotor model based on the covariant density functional theory. We show that the deformation of Si does not completely disappear, even though it is somewhat reduced, after a particle is added if the beyond-mean-field effect is taken into account. We also discuss the impurity effect of particle on the electric quadrupole transition, and show that an addition of a particle leads to a reduction in the value, as a consequence of the reduction in the deformation parameter.

    nucl-thnucl-exPRC(2018)·27 citations
  4. 04

    Pion-kaon femtoscopy in Pb--Pb collisions at TeV modeled in (3+1)D hydrodynamics coupled to Therminator 2 and the effect of delayed kaon emission

    Adam Kisiel🇵🇱

    Non-identical particle femtoscopy measures the size of the system emitting particles ("radius") in heavy-ion collisions as well as the difference between mean emission space-time coordinates of two particle species ("emission asymmetry"). The system created in such collisions at the LHC behaves collectively and its dynamics is well described by hydrodynamic models. A significant emission asymmetry between pions and kaons, coming from collective flow, enhanced by contribution from flowing resonances is predicted. We present calculations within the (3+1)D viscous hydrodynamic model coupled to statistical hadronization code Therminator 2, corresponding to Pb--Pb collisions at TeV. We obtain femtoscopic radii and emission asymmetry for pion-kaon pairs as a function of collision centrality. The radii grow linearly with cube root of particle multiplicity density. The emission asymmetry is negative and comparable to the radius, indicating that pions are emitted closer to the center of the system and/or later than kaons. Recent ALICE Collaboration measurements of identical kaon femtoscopy shows that kaons are emitted, on average, 2.1~fm/ later than pions. We modify our calculation by introducing such delay and find that the system source size is only weakly affected. In contrast the pion-kaon emission asymmetry is directly sensitive to such delays and the modified calculation shows significantly lower values of asymmetry. Therefore we propose the measurement of the pion-kaon femtoscopic correlation function as a sensitive probe of the time delays in particle emission.

    nucl-thhep-exnucl-exPRC(2018)·18 citations
  5. 05

    A quasi-particle model with a phenomenological critical point

    Hong-Hao Ma🇧🇷 · Danuce Marcele Dudek🇧🇷 · Kai Lin🇧🇷 · Wei-Liang Qian🇧🇷 · Yogiro Hama🇧🇷 · Takeshi Kodama🇧🇷

    A hybrid parameterization of a quasiparticle equation of state is proposed, with a critical point implemented phenomenologically. On the one hand, a quasiparticle model with finite chemical potential is employed for the quark-gluon plasma phase, calibrated to the lattice quantum chromodynamics data. On the other hand, the low-temperature region for the hadronic phase of the matter is described by the hadronic resonance gas model with excluded volume correction. A particular interpolation scheme is adopted so that the phase transition is a smooth crossover for small chemical potential. A phenomenological critical pointed is implemented beyond which the phase transition becomes that of the first order.

    nucl-th1 citation

Affiliations

first authorsco-authorsvia INSPIRE