PaperPanorama

Nuclear Theory·nucl-th

Monday·November 14, 2022

8 papers3 primary·5 cross-listed

  1. 04

    Geometric confinement in gauge theories

    Alexander D. Popov🇩🇪

    In 1978, Friedberg and Lee introduced the phenomenological soliton bag model of hadrons, generalizing the MIT bag model developed in 1974 shortly after the formulation of QCD. In this model, quarks and gluons are confined due to coupling with a real scalar field which tends to zero outside some compact region determined dynamically from the equations of motion. The gauge coupling in the soliton bag model is running as the inverse power of already at the semiclassical level. We show that this model arises naturally as a consequence of introducing the warped product metric on the principal -bundle with a non-Abelian group over Minkowski space . Confinement of quarks and gluons in a compact domain is a consequence of the collapse of the bundle manifold to outside due to shrinking of the group manifold to a point. We describe the formation of such regions as a dynamical process controlled by the order parameter field .

    hep-thhep-lathep-phnucl-thSymmetry(2023)·1 citation
  2. 05

    A fast-rotating pear-shaped nucleus

    A. Karmakar · P. Datta · Soumik Bhattacharya · Shabir Dar · S. Bhattacharya · G. Mukherjee · H. Pai · S. Basu · S. Nandi · S. S. Nayak · Sneha Das · R. Raut and 6 other authors

    The spectroscopic studies have identified few Actinide and Lanthanide nuclei of the periodic table, which can assume the pear shape. The low frequency collective rotation of these nuclei has been established by determining the band structure of the excited levels and their gamma decay rates. In this article, we report the rotation of a pear-shaped nucleus in 100 Ru, which rotates nearly three times faster than the previously known cases. The three novel consequences of this fast rotation are: the realization of a pear-shape in an excited state, its moment of inertia becoming a constant of motion and its shape evolution. These inferences have been arrived at by comparing the characteristics of the rotational band of 100 Ru with three of the best-known examples of a rotating pear-shaped nucleus and through the theoretical interpretation of the data. The observation of a pear-shaped nucleus in the lighter mass region opens up the possibility of a systematic study of the effects of fast rotation on this shape.

    nucl-exnucl-th0 citations
  3. 06

    Zooming in on Multiquark Hadrons within QCD Sum-Rule Approaches

    Wolfgang Lucha🇦🇹 · Dmitri Melikhov🇷🇺 · Hagop Sazdjian🇫🇷

    Aiming at self-consistent descriptions of multiquark hadrons (such as tetraquarks, pentaquarks, hexaquarks) by means of QCD sum rules, we note that the totality of contributions to two-point or three-point correlation functions that involve, respectively, either two or just a single operator capable of interpolating the particular multiquark under study can be straightforwardly disentangled into two disjoint classes defined by unambiguously identifiable members. The first is formed by so-called multiquark-phile contributions which indeed might support multiquarks. In the case of flavour-exotic tetraquarks, by definition composed of four (anti-) quarks of mutually different flavours, a tetraquark-phile contribution has to exhibit two or more gluon exchanges of appropriate topology. The second consists of contributions evidently not bearing any relation to multiquarks; these must be discarded when studying multiquarks by QCD sum rules. The first class only should enter the "multiquark-adequate" QCD sum rules for exotic hadrons.

    hep-phnucl-thEPJ Web Conf.(2022)·0 citations
  4. 07

    The impact of fluctuating initial conditions on bottomonium suppression in 5.02 TeV heavy-ion collisions

    Huda Alalawi🇺🇸 · Jacob Boyd🇺🇸 · Chun Shen🇺🇸 · Michael Strickland🇺🇸

    We compute bottomonium suppression and elliptic flow within the pNRQCD effective field theory using an open quantum systems approach. For the hydrodynamical background, we use 2+1D MUSIC second-order viscous hydrodynamics with IP-Glasma initial conditions and evolve bottom/antibottom quantum wave packets in real time in these backgrounds. We find that the impact of fluctuating initial conditions is small when compared to results obtained using smooth initial conditions. Including the effect of fluctuating initial conditions, we find that the Upsilon(1S) integrated elliptic flow is v_2[1S] = 0.005 +/- 0.002 +/- 0.001, with the first and second variations corresponding to statistical and systematic theoretical uncertainties, respectively.

    hep-phnucl-thPRC(2023)·12 citations
  5. 08

    On the Infinite Variance Problem in Fermion Models

    Andrei Alexandru🇺🇸 · Paulo Bedaque🇺🇸 · Andrea Carosso🇺🇸 · Hyunwoo Oh🇺🇸

    Monte Carlo calculations of fermionic systems with continuous auxiliary fields frequently suffer from a diverging variance. If a system has the infinite variance problem, one cannot estimate observables reliably even with an infinite number of samples. In this paper, we explore a method to deal with this problem based on sampling according to the distribution of a system with an extra time-slice. The necessary reweighting factor is computed both perturbatively and through a secondary Monte Carlo. We show that the Monte Carlo reweigthing coupled to the use of a non-biased estimator of the reweigthing factor leads to a method that eliminates the infinite variance problem at a very small extra cost. We compute the double occupancy in the Hubbard model at half-filling to demonstrate the method and compare the results to well established results obtained by other methods.

    hep-latcond-mat.str-elnucl-thPRD(2023)·7 citations

Affiliations

first authorsco-authorsvia INSPIRE