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Light quark masses in N_f = 2+1 lattice QCD with Wilson fermions

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arxiv 1911.08025 v3 pith:P745SORP submitted 2019-11-19 hep-lat

classification hep-lat
keywords improvedlatticemassesnon-perturbativelyquarkactionknownlight
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

We present a lattice QCD determination of light quark masses with three sea-quark flavours ($N_f = 2+1$). Bare quark masses are known from PCAC relations in the framework of CLS lattice computations with a non-perturbatively improved Wilson-Clover action and a tree-level Symanzik improved gauge action. They are fully non-perturbatively improved, including the recently computed Symanzik counter-term $b_{\rm A} - b_{\rm P}$. The mass renormalisation at hadronic scales and the renormalisation group running over a wide range of scales are known non-perturbatively in the Schr\"odinger functional scheme. In the present paper we perform detailed extrapolations to the physical point, obtaining (for the four-flavour theory) $m_{u/d}(2{\rm GeV}) = 3.54(12)(9)$ MeV and $m_s(2{\rm GeV}) = 95.7(2.5)(2.4)$ MeV in the $\bar{MS}$ scheme. For the mass ratio we have $m_s/m_{u/d} = 27.0(1.0)(0.4)$. The RGI values in the three-flavour theory are $M_{u/d} = 4.70(15)(12)$ MeV and $M_s = 127.0(3.1)(3.2)$ MeV.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Impact of Dynamical Charm Quark and Mixed Action Effect on Light Hadron Masses and Decay Constants

    hep-lat 2026-03 conditional novelty 6.0 of 10

    A dynamical charm quark does not measurably change light-hadron masses or decay constants, and a clover-on-HISQ mixed action reduces O(a^2) discretization errors in the continuum limit.

  2. On the contribution from the light quarks to $H\to\gamma\gamma , \gamma Z$

    hep-ph 2025-07 conditional novelty 6.0 of 10

    The light-quark contribution to H to gamma gamma and H to gamma Z is nonzero and linear in quark masses, with a large enhancement in the two-photon channel.

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