PaperPanorama

Nuclear Theory·nucl-th

Wednesday·August 2, 2017

11 papers6 primary·5 cross-listed

  1. 01

    Relating centrality to impact parameter in nucleus-nucleus collisions

    Sruthy Jyothi Das🇫🇷 · Giuliano Giacalone🇫🇷 · Pierre-Amaury Monard🇫🇷 · Jean-Yves Ollitrault🇫🇷

    In ultrarelativistic heavy-ion experiments, one estimates the centrality of a collision by using a single observable, say , typically given by the transverse energy or the number of tracks observed in a dedicated detector. The correlation between and the impact parameter, , of the collision is then inferred by fitting a specific model of the collision dynamics, such as the Glauber model, to experimental data. The goal of this paper is to assess precisely which information about can be extracted from data without any specific model of the collision. Under the sole assumption that the probability distribution of for a fixed is Gaussian, we show that the probability distribution of the impact parameter in a narrow centrality bin can be accurately reconstructed up to centrality. We apply our methodology to data from the Relativistic Heavy Ion Collider and the Large Hadron Collider. We propose a simple measure of the precision of the centrality determination, which can be used to compare different experiments.

    nucl-thhep-phnucl-exPRC(2018)·72 citations
  2. 02

    Introduction of the one-body correlation operator in the unitary-model-operator approach

    Takayuki Miyagi · Takashi Abe · Ryoji Okamoto · Takaharu Otsuka

    In the earlier unitary-model-operator approach (UMOA), one-body correlations have been taken into account approximately by the diagonalization of unitary-transformed Hamiltonians in the and space. With this prescription, the dependence of the harmonic-oscillator energy () on calculated observables is not negligible even at larger model spaces. In the present work, we explicitly introduce the one-body correlation operator so that it optimizes the single-particle basis states and then reduces the -dependence. For an actual demonstration, we calculate the energy and radius for the He ground state with the softened nucleon-nucleon () interactions from Argonne v18 (AV18) and chiral effective field theory (EFT) up to the next-to-next-to-next leading order (NLO). As a result, we obtain practically -free results at sufficiently large model spaces. The present results are reasonably close to those by the other ab initio calculations with the same interactions. This methodological development enables us more systematic analysis of calculation results in the UMOA. We also discuss qualitatively the origin of the -dependence on calculated observables in a somewhat simplified way.

    nucl-thPRC(2017)·4 citations
  3. 03

    Neutrino-nucleus cross sections in and with KDAR neutrinos

    F Akbar🇮🇳 · M. Sajjad Athar🇮🇳 · S. K. Singh🇮🇳

    High intensity monoenergetic muon neutrinos of energy 236 MeV from kaon decay at rest (KDAR) at the medium energy proton accelerator facilities like J-PARC and Fermilab are proposed to be used for making precision measurements of neutrino-nucleus cross sections in and and perform neutrino oscillation experiments in and modes. In view of these developments, we study the theoretical uncertainties arising due to the nuclear medium effects in the neutrino-nucleus cross sections as well as in the angular and energy distributions of the charged leptons produced in the charged current (CC) induced reactions by and in and in the energy region of 300 MeV. The calculations have been done in a microscopic model using the local density approximation which takes into account the nuclear effects due to the Fermi motion, binding energy and long range correlations. The results are compared with the other calculations available in the literature.

    nucl-thJ.Phys.G(2017)·12 citations
  4. 04

    Hollowness in pp scattering at the LHC

    Wojciech Broniowski🇵🇱 · Enrique Ruiz Arriola🇪🇸

    We examine how the effect of hollowness in pp scattering at the LHC (minimum of the inelasticity profile at zero impact parameter) depends on modeling of the phase of the elastic scattering amplitude as a function of the momentum transfer. We study the cases of the constant phase, the Bailly, and the so called standard parameterizations. It is found that the 2D hollowness holds in the first two cases, whereas the 3D hollowness is a robust effect, holding for all explored cases.

    nucl-thhep-exhep-phActa Phys.Polon.Supp.(2017)·14 citations
  5. 05

    A Study of Multi hypernuclei within Spherical Relativistic Mean-field Approach

    Asloob A. Rather · M. Ikram · A. A. Usmani · Bharat Kumar · S. K. Patra

    This research article is a follow up of earlier work by M. Ikram et al., reported in International Journal of Modern Physics E {\bf{25}}, 1650103 (2016) wherein we searched for magic numbers in experimentally confirmed doubly magic nucleonic cores in light to heavy mass region (ie.) by injecting 's into them. In present manuscript, working within the state-of-art relativistic mean field theory with inclusion of and interaction in hypernuclei using the predicted doubly magic nucleonic cores ie. 120, 120, 132, 132, 138, 138 of elusive superheavy mass regime. In analogy to well established signatures of magicity in conventional nuclear theory, the prediction of hypernuclear magicity are made on the basis of one-, two- separation energy () and two lambda shell gaps () in multi- hypernuclei. The calculations suggest that the numbers 92, 106, 126, 138, 184, 198, 240, and 258 might be the shell closures after introducing the 's in elusive superheavy nucleonic cores. Moreover, in support of shell closure the investigation of pairing energy and effective pairing gap has also been made. The appearance of new lambda shell closures other than the nucleonic ones predicted by various relativistic and non-relativistic theoretical investigations can be attributed to the relatively weak strength of spin-orbit coupling in hypernuclei compared to normal nuclei.

    nucl-thBraz.J.Phys.(2017)·0 citations
  6. 06

    "Luneburg-lens-like structural Pauli attractive core of the nuclear force at short distances" [arXiv:1703.09396]

    Gerald A. Miller

    A recent paper [S. Ohkubo, Phys. Rev. C 95, 044002 (2017)] found that the measured 1S0 phase shifts can be reproduced using a deeply attractive nucleon-nucleon potential. We find that the deuteron would decay strongly via pion emission to the deeply bound state arising in this potential. There- fore the success of a deeply attractive potential in describing phase shifts must be regarded only as an interesting curiosity.

    nucl-thNPA(2018)·0 citations
  7. 07

    On the importance of viscous dissipation and heat conduction in binary neutron-star mergers

    Mark G. Alford · Luke Bovard · Matthias Hanauske · Luciano Rezzolla · Kai Schwenzer

    Inferring the properties of dense matter is one of the most exciting prospects from the measurement of gravitational waves from neutron star mergers. However, it will require reliable numerical simulations that incorporate viscous dissipation and energy transport if these can play a significant role within the survival time of the post-merger object. We calculate timescales for typical forms of dissipation and find that thermal transport and shear viscosity will not be important unless neutrino trapping occurs, which requires temperatures above about 10 MeV and gradients over lengthscales of 0.1 km or less. On the other hand, if direct-Urca processes remain suppressed, leaving modified-Urca processes to establish flavor equilibrium, then bulk viscous dissipation could provide significant damping to density oscillations observed right after the merger. When comparing with data from a state-of-the-art merger simulation we find that the bulk viscosity takes values close to its resonant maximum in a typical neutron-star merger, motivating a more careful assessment of the role of bulk viscous dissipation in the gravitational-wave signal from merging neutron stars.

    gr-qcastro-ph.HEnucl-thPRL(2018)·248 citations
  8. 08

    Study of Minor Actinides Transmutation in PWR MOX fuel

    Shengli Chen · Cenxi Yuan · Jingxia Wu · Yaolei Zou

    The management of long-lived radionuclides in spent fuel is a key issue to achieve the closed nuclear fuel cycle and the sustainable development of nuclear energy. Partitioning-Transmutation is supposed to be an efficient method to treat the long-lived radionuclides in spent fuel. Some Minor Actinides (MAs) have very long half-lives among the radionuclides in the spent fuel. Accordingly, the study of MAs transmutation is a significant work for the post-processing of spent fuel. In the present work, the transmutations in Pressurized Water Reactor (PWR) mixed oxide (MOX) fuel are investigated through the Monte Carlo based code RMC. Two kinds of MAs, Np and five MAs (Np, Am, Am, Cm and Cm) are incorporated homogeneously into the MOX fuel assembly. The transmutation of MAs is simulated with different initial MOX concentrations. The results indicate an overall nice efficiency of transmutation in both initial MOX concentrations, especially for the two kinds of MAs primarily generated in the UOX fuel, Np and Am. In addition, the inclusion of Np in MOX has no large influence for other MAs, while the transmutation efficiency of Np is excellent. The transmutation of MAs in MOX fuel depletion is expected to be a new, efficient nuclear spent fuel management method for the future nuclear power generation.

    physics.app-phnucl-thICONE25-66250, 2017 (Proceedings of the 2…·0 citations
  9. 09

    Squeezing the Efimov effect

    J. H. Sandoval · F. F. Bellotti · M. T. Yamashita · T. Frederico · D. V. Fedorov · A. S. Jensen · N. T. Zinner

    The quantum mechanical three-body problem is a source of continuing interest due to its complexity and not least due to the presence of fascinating solvable cases. The prime example is the Efimov effect where infinitely many bound states of identical bosons can arise at the threshold where the two-body problem has zero binding energy. An important aspect of the Efimov effect is the effect of spatial dimensionality; it has been observed in three dimensional systems, yet it is believed to be impossible in two dimensions. Using modern experimental techniques, it is possible to engineer trap geometry and thus address the intricate nature of quantum few-body physics as function of dimensionality. Here we present a framework for studying the three-body problem as one (continuously) changes the dimensionality of the system all the way from three, through two, and down to a single dimension. This is done by considering the Efimov favorable case of a mass-imbalanced system and with an external confinement provided by a typical experimental case with a (deformed) harmonic trap.

    cond-mat.quant-gasnucl-thquant-phJ.Phys.B(2018)·18 citations
  10. 10

    Probing the Efimov discrete scaling in atom-molecule collision

    M. A. Shalchi · M. T. Yamashita · M. R. Hadizadeh · E. Garrido · Lauro Tomio · T. Frederico

    The discrete Efimov scaling behavior, well-known in the low-energy spectrum of three-body bound systems for large scattering lengths (unitary limit), is identified in the energy dependence of atom-molecule elastic cross-section in mass imbalanced systems. That happens in the collision of a heavy atom with mass with a weakly-bound dimer formed by the heavy atom and a lighter one with mass . Approaching the heavy-light unitary limit the wave elastic cross-section will present a sequence of zeros/minima at collision energies following closely the Efimov geometrical law. Our results open a new perspective to detect the discrete scaling behavior from low-energy scattering data, which is timely in view of the ongoing experiments with ultra-cold binary mixtures having strong mass asymmetries, such as Lithium and Caesium or Lithium and Ytterbium.

    physics.atom-phcond-mat.quant-gasnucl-thquant-phPRA(2018)·8 citations
  11. 11

    Kosterlitz-Thouless transition and vortex-antivortex lattice melting in two-dimensional Fermi gases with - or -wave pairing

    Gaoqing Cao · Lianyi He · Xu-Guang Huang

    We present a theoretical study of the finite-temperature Kosterlitz-Thouless (KT) and vortex-antivortex lattice (VAL) melting transitions in two-dimensional Fermi gases with - or -wave pairing. For both pairings, when the interaction is tuned from weak to strong attractions, we observe a quantum phase transition from the Bardeen-Cooper-Schrieffer (BCS) superfluidity to the Bose-Einstein condensation (BEC) of difermions. The KT and VAL transition temperatures increase during this BCS-BEC transition and approach constant values in the deep BEC region. The BCS-BEC transition is characterized by the non-analyticities of the chemical potential, the superfluid order parameter, and the sound velocities as functions of the interaction strength at both zero and finite temperatures; however, the temperature effect tends to weaken the non-analyticities comparing to the zero temperature case. The effect of mismatched Fermi surfaces on the -wave pairing is also studied.

    cond-mat.quant-gasnucl-thquant-phPRA(2017)·1 citation

Affiliations

first authorsco-authorsvia INSPIRE