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Can we observe the QCD phase transition-generated gravitational waves through pulsar timing arrays?
KTH, Centres, Nordic Institute for Theoretical Physics NORDITA.ORCID iD: 0000-0002-7304-021X
Carnegie Mellon Univ, McWilliams Ctr Cosmol, Pittsburgh, PA 15213 USA.;Carnegie Mellon Univ, Dept Phys, Pittsburgh, PA 15213 USA..
KTH, Centres, Nordic Institute for Theoretical Physics NORDITA. KTH Royal Inst Technol, NORDITA, S-10691 Stockholm, Sweden.;Stockholm Univ, S-10691 Stockholm, Sweden.;Stockholm Univ, AlbaNova Univ Ctr, Dept Astron, S-10691 Stockholm, Sweden..
Ilia State Univ, Fac Nat Sci & Med, GE-0194 Tbilisi, Georgia.;Carnegie Mellon Univ, McWilliams Ctr Cosmol, Pittsburgh, PA 15213 USA.;Carnegie Mellon Univ, Dept Phys, Pittsburgh, PA 15213 USA.;Abastumani Astrophys Observ, GE-0179 Tbilisi, Georgia.;Laurentian Univ, Dept Phys, Sudbury, ON P3E 2C, Canada..
2021 (English)In: Physical Review D: covering particles, fields, gravitation, and cosmology, ISSN 2470-0010, E-ISSN 2470-0029, Vol. 104, no 4, article id 043513Article in journal (Refereed) Published
Abstract [en]

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 10(-9) 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.

Place, publisher, year, edition, pages
American Physical Society (APS) , 2021. Vol. 104, no 4, article id 043513
National Category
Astronomy, Astrophysics and Cosmology
Identifiers
URN: urn:nbn:se:kth:diva-300848DOI: 10.1103/PhysRevD.104.043513ISI: 000686912500002Scopus ID: 2-s2.0-85110972724OAI: oai:DiVA.org:kth-300848DiVA, id: diva2:1598065
Note

QC 20210928

Available from: 2021-09-28 Created: 2021-09-28 Last updated: 2022-06-25Bibliographically approved

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Brandenburg, AxelHe, Yutong

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