Calculation of the axion mass based on high-temperature lattice quantum chromodynamics
By S. Borsányi, Zoltán Fodor, J. Guenther, K. Kampert, Sándor D. Katz, T. Kawanai, T. Kovács, S. Mages, Attila Pásztor, F. Pittler and 3 more. Nature, 2016
764 citations recorded by the source corpus.
Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/5dc883ea0d234cfb8727f4e8c21aa0241f30f95e
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In Astronomy and Astrophysics
- J. Redondo
- A. Ringwald
- Igor G. Irastorza
- M. Cicoli
- G. Ghisellini
- C. Byrnes
- F. Tavecchio
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In Nuclear and High Energy Physics
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- Igor G. Irastorza
- M. Cicoli
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- Maurizio Giannotti
- Zoltán Fodor
- Sándor D. Katz
Citations in the corpus
- More axions from strings (2020, background): “where, as suggested by the dilute instanton gas approximation [37] and supported by recent lattice simulations [38–42] (see also ref.”
- QCD axion window and low-scale inflation (2018, positive): “08 [34], and we adopt TQCD ' 153 MeV and χ0 ' (75.”
- The landscape of QCD axion models (2020, methodology): “A direct calculation of the topological susceptibility via QCD lattice techniques finds a similar central value, with an error five time larger [117].”
- Early seeds of axion miniclusters (2018, methodology): “Axion models with values of fA 108 GeV are ruled out because many stellar systems would cool faster than observed by the emission of axions (see [6] and the recent revisions [7–10]).”
- Improved axion emissivity from a supernova via nucleon-nucleon bremsstrahlung (2019, background): “The axion mass is given by [5, 6] ma = 5.”
- Recent Progress in the Physics of Axions and Axion-Like Particles (2020, background): “(2.28)) and ma(tosc)/ma(t0) ≈ 6× 10−4(GeV/Tosc)n (n ' 4) for Tosc & 150 MeV [48], where mπ and fπ are the pion mass and the pion decay constant, respectively, and Tosc is the temperature at t = tosc.”
- Leading hadronic contribution to the muon magnetic moment from lattice QCD (2020, methodology): “ent renormalization factor as Z V = [(T=4) (3T=4)] 1. The plot shows data from a = 3:7753 ensemble, T= 56. This version of the operator has been extensively used in previous thermodynamical studies [15,16]. We apply O(a) improvement to the overlap propagator by transforming each instance of D 1 ov (”
- The dark-matter axion mass (2017, background): “have presented [1] results up to and beyond the relevant temperature range.”
- Physics potential of the International Axion Observatory (IAXO) (2019, methodology): “75 (see [86]) the latter figure being applicable at very early times when even the top quark was in thermal equilibrium.”