PaperPanorama

Nuclear Theory·nucl-th

Thursday·November 24, 2022

10 papers4 primary·6 cross-listed

  1. 05

    Width effects of broad new resonances in loop observables and application to

    Andreas Crivellin🇨🇭 · Martin Hoferichter🇨🇭

    In the phenomenology of strong interactions most physical states acquire a substantial width, and thus can only be defined in a model-independent way by pole positions and residues of the -matrix. This information is incorporated in the Källén-Lehmann representation, whose spectral function characterizes the shape of the resonance and can be constrained by the dominant decay channels. Here, we argue that similar effects become important whenever beyond-the-Standard-Model particles possess a sizable decay width - as possible for instance in cases with a large branching fraction to a dark sector or strongly coupled scenarios - and show how their widths can be incorporated in the calculation of loop observables. As an application, we consider the anomalous magnetic moment of the muon, including both the direct effect of new physics and the possible indirect impact of a broad light on cross sections. Throughout, we provide results for a general spectral function and its reconstruction from the one-loop imaginary part, where the latter captures the leading two-loop effects.

    hep-phhep-exhep-latnucl-thPRD(2023)·29 citations
  2. 06

    Schwinger mechanism for gluons from lattice QCD

    A. C. Aguilar🇧🇷 · F. De Soto🇪🇸 · M. N. Ferreira🇪🇸 · J. Papavassiliou🇪🇸 · F. Pinto-Gómez🇪🇸 · C. D. Roberts🇨🇳 · J. Rodríguez-Quintero🇪🇸

    Continuum and lattice analyses have revealed the existence of a mass-scale in the gluon two-point Schwinger function. It has long been conjectured that this expresses the action of a Schwinger mechanism for gauge boson mass generation in quantum chromodynamics (QCD). For such to be true, it is necessary and sufficient that a dynamically-generated, massless, colour-carrying, scalar gluon+gluon correlation emerge as a feature of the dressed three-gluon vertex. Working with results on elementary Schwinger functions obtained via the numerical simulation of lattice-regularised QCD, we establish with an extremely high level of confidence that just such a feature appears; hence, confirm the conjectured origin of the gluon mass scale.

    hep-phhep-exhep-latnucl-ex+1PLB(2023)·37 citations
  3. 07

    Subleading power corrections to heavy quarkonium production in QCD factorization approach

    Kyle Lee🇺🇸 · Jian-Wei Qiu🇺🇸 · George Sterman🇺🇸 · Kazuhiro Watanabe🇫🇷

    We report the current understanding of heavy quarkonium production at high transverse momentum () in hadronic collisions in terms of QCD factorization. In this presentation, we highlight the role of subleading power corrections to heavy quarkonium production, which are essential to describe the spectrum of quarkonium at a relatively lower . We also introduce prescription to match QCD factorization to fixed-order NRQCD factorization calculations for quarkonium production at low .

    hep-phnucl-thEPJ Web Conf.(2022)·5 citations
  4. 08

    Spin polarization and alignment in heavy-ion collisions

    Subhash Singha🇨🇳

    We report the measurements of global spin polarization of hyperons () from FAIR, RHIC and LHC energies. The continue to follow an increasing trend at < 7.7 GeV indicating that enormous vorticity prevail even in hadronic dominant region. New measurements of local spin polarization () from isobar collisions follow the same pattern observed in previous RHIC and LHC energies. An observable motivated by predicted baryonic Spin Hall Effect, the net local polarization (), shows negative value in Au+Au collisions at = 19.6 and 27 GeV. The first measurement with respect to third order harmonic in 200 GeV RHIC isobar collisions show a non-zero sine modulation, indicating the presence of complex vortical structure in the medium. Surprising new patterns of spin alignment () for various vector mesons (, , and ) emerged at both RHIC and LHC energies. The large deviation in of several species poses challenge to the theory.

    nucl-exhep-exhep-phnucl-thEPJ Web Conf.(2023)·2 citations
  5. 09

    Phase transition amplification of proton number fluctuations in nuclear collisions from a transport model approach

    O. Savchuk🇺🇸 · R. V. Poberezhnyuk🇺🇦 · A. Motornenko🇩🇪 · J. Steinheimer🇩🇪 · M. I. Gorenstein🇺🇦 · V. Vovchenko🇺🇸

    The time evolution of particle number fluctuations in nuclear collisions at intermediate energies ( GeV) is studied by means of the UrQMD-3.5 transport model. The transport description incorporates baryonic interactions through a density-dependent potential. This allows for an implementation of a first order phase transition including a mechanically unstable region at large baryon density. The scaled variance of the baryon and proton number distributions is calculated in the central cubic spatial volume of the collisions at different times. A significant enhancement of fluctuations associated with the unstable region is observed. This enhancement persists to late times reflecting a memory effect for the fluctuations. The presence of the phase transition has a much smaller influence on the observable event-by-event fluctuations of protons in momentum space.

    hep-phnucl-thPRC(2023)·14 citations
  6. 10

    Transverse-momentum-dependent factorization at next-to-leading power

    Leonard Gamberg🇺🇸 · Zhong-Bo Kang🇺🇸 · Ding Yu Shao🇨🇳 · John Terry🇺🇸 · Fanyi Zhao🇺🇸

    We study transverse momentum dependent factorization and resummation at sub-leading power in Drell-Yan and semi-inclusive deep inelastic scattering. In these processes the sub-leading power contributions to the cross section enter as a kinematic power correction to the leptonic tensor, and the kinematic, intrinsic, and dynamic sub-leading contributions to the hadronic tensor. By consistently treating the power counting of the interactions, we demonstrate renormalization group consistency. We calculate the anomalous dimensions of the kinematic and intrinsic sub-leading correlation functions at one loop and find that the evolution equations give rise to anomalous dimension matrices which mix leading and sub-leading power distribution functions. Additionally we calculate the hard and soft functions associated with each of these contributions. We find that these hard and soft contributions differ from those at the leading power. Finally, we calculate the rapidity anomalous dimension for the dynamic sub-leading distributions and find that it is the same as the leading power anomalous dimension. We then comment on the implications for the soft function associated with this contribution. Using this information, we establish the factorization formalism at sub-leading power for these processes at the one-loop level.

    hep-phnucl-exnucl-th30 citations

Affiliations

first authorsco-authorsvia INSPIRE