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    Can we observe the QCD phase transition-generated gravitational waves through pulsar timing arrays?

    Axel Brandenburg1,2,3,4,*, Emma Clarke4,†, Yutong He1,2,‡, and Tina Kahniashvili4,3,5,6,§

    • 1Nordita, KTH Royal Institute of Technology and Stockholm University, 10691 Stockholm, Sweden
    • 2Department of Astronomy, AlbaNova University Center, Stockholm University, 10691 Stockholm, Sweden
    • 3Faculty of Natural Sciences and Medicine, Ilia State University, 0194 Tbilisi, Georgia
    • 4McWilliams Center for Cosmology and Department of Physics, Carnegie Mellon University, Pittsburgh, Pennsylvania 15213, USA
    • 5Abastumani Astrophysical Observatory, Tbilisi, GE-0179, Georgia
    • 6Department of Physics, Laurentian University, Sudbury, Ontario P3E 2C, Canada

    • *brandenb@nordita.org
    • emmaclar@andrew.cmu.edu
    • yutong.he@su.se
    • §tinatin@andrew.cmu.edu

    Phys. Rev. D 104, 043513 – Published 11 August, 2021

    DOI: https://doi.org/10.1103/PhysRevD.104.043513

    Abstract

    We perform numerical simulations of gravitational waves (GWs) induced by hydrodynamic and hydromagnetic turbulent sources that might have been present at cosmological quantum chromodynamic (QCD) phase transitions. For turbulent energies of about 4% of the radiation energy density, the typical scale of such motions may have been a sizable fraction of the Hubble scale at that time. The resulting GWs are found to have an energy fraction of about 109 of the critical energy density in the nHz range today and may already have been observed by the NANOGrav Collaboration. This is further made possible by our findings of shallower spectra proportional to the square root of the frequency for nonhelical hydromagnetic turbulence. This implies more power at low frequencies than for the steeper spectra previously anticipated. The behavior toward higher frequencies depends strongly on the nature of the turbulence. For vortical hydrodynamic and hydromagnetic turbulence, there is a sharp drop of spectral GW energy by up to five orders of magnitude in the presence of helicity, and somewhat less in the absence of helicity. For acoustic hydrodynamic turbulence, the sharp drop is replaced by a power law decay, albeit with a rather steep slope. Our study supports earlier findings of a quadratic scaling of the GW energy with the magnetic energy of the turbulence and inverse quadratic scaling with the peak frequency, which leads to larger GW energies under QCD conditions.

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