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| 001 | 12187 | ||
| 005 | 20210129210553.0 | ||
| 024 | 7 | _ | |2 DOI |a 10.1016/j.physletb.2011.05.053 |
| 024 | 7 | _ | |2 WOS |a WOS:000292993900014 |
| 024 | 7 | _ | |a altmetric:15738842 |2 altmetric |
| 037 | _ | _ | |a PreJuSER-12187 |
| 041 | _ | _ | |a eng |
| 082 | _ | _ | |a 530 |
| 084 | _ | _ | |2 WoS |a Physics, Multidisciplinary |
| 100 | 1 | _ | |0 P:(DE-HGF)0 |a Durr, S. |b 0 |
| 245 | _ | _ | |a Lattice QCD at the physical point: Light quark masses |
| 260 | _ | _ | |a Amsterdam |b North-Holland Publ. |c 2011 |
| 300 | _ | _ | |a 265 - 268 |
| 336 | 7 | _ | |a Journal Article |0 PUB:(DE-HGF)16 |2 PUB:(DE-HGF) |
| 336 | 7 | _ | |a Output Types/Journal article |2 DataCite |
| 336 | 7 | _ | |a Journal Article |0 0 |2 EndNote |
| 336 | 7 | _ | |a ARTICLE |2 BibTeX |
| 336 | 7 | _ | |a JOURNAL_ARTICLE |2 ORCID |
| 336 | 7 | _ | |a article |2 DRIVER |
| 440 | _ | 0 | |0 4934 |a Physics Letters B |v 701 |x 0370-2693 |y 2 |
| 500 | _ | _ | |a We used HPC resources from FZ Julich and from GENCI[IDRIS/CCRT] grant 52275, as well as clusters at Wuppertal and CPT. This work is supported in part by EU grants I3HP, FP7/2007-2013/ERC No. 208740, MRTN-CT-2006-035482 (FLAVIAnet), DFG grants FO 50212, SFB-TR 55 and CNRS grants GDR 2921 and PICS 4707. |
| 520 | _ | _ | |a Ordinary matter is described by six fundamental parameters: three couplings (gravitational, electromagnetic and strong) and three masses: the electron's (m(e)) and those of the up (m(u)) and down (m(d)) quarks. An additional mass enters through quantum fluctuations: the strange quark mass (m(s)). The three couplings and m(e) are known with an accuracy of better than a few per mil. Despite their importance, m(u), m(d) (their average m(ud)) and m(s) are far less accurately known. Here we determine them with a precision below 2% by performing ab initio lattice quantum chromodynamics (QCD) calculations, in which all systematics are controlled. We use pion and quark masses down to (and even below) their physical values, lattice sizes of up to 6 fm, and five lattice spacings to extrapolate to continuum spacetime. All necessary renormalizations are performed nonperturbatively. (C) 2011 Elsevier B.V. All rights reserved. |
| 536 | _ | _ | |0 G:(DE-Juel1)FUEK411 |2 G:(DE-HGF) |x 0 |c FUEK411 |a Scientific Computing (FUEK411) |
| 536 | _ | _ | |a 411 - Computational Science and Mathematical Methods (POF2-411) |0 G:(DE-HGF)POF2-411 |c POF2-411 |x 1 |f POF II |
| 536 | _ | _ | |a QCDTHERMO - QCD thermodynamics on the lattice (208740) |0 G:(EU-Grant)208740 |c 208740 |x 2 |f ERC-2007-StG |
| 588 | _ | _ | |a Dataset connected to Web of Science |
| 650 | _ | 7 | |2 WoSType |a J |
| 653 | 2 | 0 | |2 Author |a Quark masses |
| 653 | 2 | 0 | |2 Author |a Lattice QCD |
| 700 | 1 | _ | |0 P:(DE-HGF)0 |a Fodor, Z. |b 1 |
| 700 | 1 | _ | |0 P:(DE-HGF)0 |a Hoelbling, C. |b 2 |
| 700 | 1 | _ | |0 P:(DE-HGF)0 |a Katz, S.D. |b 3 |
| 700 | 1 | _ | |0 P:(DE-Juel1)132171 |a Krieg, S. |b 4 |u FZJ |
| 700 | 1 | _ | |0 P:(DE-HGF)0 |a Kurth, T. |b 5 |
| 700 | 1 | _ | |0 P:(DE-HGF)0 |a Lellouch, L. |b 6 |
| 700 | 1 | _ | |0 P:(DE-Juel1)132179 |a Lippert, T. |b 7 |u FZJ |
| 700 | 1 | _ | |0 P:(DE-HGF)0 |a Szabo, K.K. |b 8 |
| 700 | 1 | _ | |0 P:(DE-HGF)0 |a Vulvert, G. |b 9 |
| 773 | _ | _ | |0 PERI:(DE-600)1466612-1 |a 10.1016/j.physletb.2011.05.053 |g Vol. 701, p. 265 - 268 |p 265 - 268 |q 701<265 - 268 |t Physics letters / B |v 701 |x 0370-2693 |y 2011 |
| 856 | 7 | _ | |u http://dx.doi.org/10.1016/j.physletb.2011.05.053 |
| 909 | C | O | |o oai:juser.fz-juelich.de:12187 |p openaire |p VDB |p ec_fundedresources |
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| 914 | 1 | _ | |y 2011 |
| 915 | _ | _ | |0 StatID:(DE-HGF)0010 |a JCR/ISI refereed |
| 920 | 1 | _ | |0 I:(DE-Juel1)JSC-20090406 |g JSC |k JSC |l Jülich Supercomputing Centre |x 0 |
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