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| 001 | 863701 | ||
| 005 | 20230217124234.0 | ||
| 024 | 7 | _ | |a 10.1103/PhysRevD.99.114505 |2 doi |
| 024 | 7 | _ | |a 0556-2821 |2 ISSN |
| 024 | 7 | _ | |a 1089-4918 |2 ISSN |
| 024 | 7 | _ | |a 1538-4500 |2 ISSN |
| 024 | 7 | _ | |a 1550-2368 |2 ISSN |
| 024 | 7 | _ | |a 1550-7998 |2 ISSN |
| 024 | 7 | _ | |a 2470-0010 |2 ISSN |
| 024 | 7 | _ | |a 2470-0029 |2 ISSN |
| 024 | 7 | _ | |a arXiv:1903.06487 |2 arXiv |
| 024 | 7 | _ | |a 2128/22470 |2 Handle |
| 024 | 7 | _ | |a altmetric:62433052 |2 altmetric |
| 024 | 7 | _ | |a WOS:000473023900003 |2 WOS |
| 037 | _ | _ | |a FZJ-2019-03706 |
| 082 | _ | _ | |a 530 |
| 100 | 1 | _ | |a Hasan, Nesreen |0 P:(DE-Juel1)145643 |b 0 |
| 245 | _ | _ | |a Nucleon axial, scalar, and tensor charges using lattice QCD at the physical pion mass |
| 260 | _ | _ | |a Melville, NY |c 2019 |b Inst.812068 |
| 264 | _ | 1 | |3 online |2 Crossref |b American Physical Society (APS) |c 2019-06-19 |
| 264 | _ | 1 | |3 print |2 Crossref |b American Physical Society (APS) |c 2019-06-01 |
| 336 | 7 | _ | |a article |2 DRIVER |
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| 336 | 7 | _ | |a Journal Article |b journal |m journal |0 PUB:(DE-HGF)16 |s 1565250651_19595 |2 PUB:(DE-HGF) |
| 336 | 7 | _ | |a ARTICLE |2 BibTeX |
| 336 | 7 | _ | |a JOURNAL_ARTICLE |2 ORCID |
| 336 | 7 | _ | |a Journal Article |0 0 |2 EndNote |
| 520 | _ | _ | |a We report on lattice QCD calculations of the nucleon isovector axial, scalar, and tensor charges. Our calculations are performed on two 2+1-flavor ensembles generated using a 2-HEX-smeared Wilson-clover action at the physical pion mass and lattice spacings $a\approx$ 0.116 and 0.093 fm. We use a wide range of source-sink separations - eight values ranging from roughly 0.4 to 1.4 fm on the coarse ensemble and three values from 0.9 to 1.5 fm on the fine ensemble - which allows us to perform an extensive study of excited-state effects using different analysis and fit strategies. To determine the renormalization factors, we use the nonperturbative Rome-Southampton approach and compare RI'-MOM and RI-SMOM intermediate schemes to estimate the systematic uncertainties. Our final results are computed in the MS-bar scheme at scale 2 GeV. The tensor and axial charges have uncertainties of roughly 4%, $g_T=0.972(41)$ and $g_A=1.265(49)$. The resulting scalar charge, $g_S=0.927(303)$, has a much larger uncertainty due to a stronger dependence on the choice of intermediate renormalization scheme and on the lattice spacing. |
| 536 | _ | _ | |a 511 - Computational Science and Mathematical Methods (POF3-511) |0 G:(DE-HGF)POF3-511 |c POF3-511 |f POF III |x 0 |
| 536 | _ | _ | |a The Proton radius and other aspects of nucleon structure from Lattice QCD (hmz37_20161101) |0 G:(DE-Juel1)hmz37_20161101 |c hmz37_20161101 |f The Proton radius and other aspects of nucleon structure from Lattice QCD |x 1 |
| 542 | _ | _ | |i 2019-06-19 |2 Crossref |u https://creativecommons.org/licenses/by/4.0/ |
| 588 | _ | _ | |a Dataset connected to arXivarXiv, CrossRef |
| 700 | 1 | _ | |a Green, Jeremy |0 P:(DE-HGF)0 |b 1 |
| 700 | 1 | _ | |a Meinel, Stefan |0 P:(DE-HGF)0 |b 2 |
| 700 | 1 | _ | |a Engelhardt, Michael |0 P:(DE-HGF)0 |b 3 |
| 700 | 1 | _ | |a Krieg, Stefan |0 P:(DE-Juel1)132171 |b 4 |e Corresponding author |
| 700 | 1 | _ | |a Negele, John |0 P:(DE-HGF)0 |b 5 |
| 700 | 1 | _ | |a Pochinsky, Andrew |0 P:(DE-HGF)0 |b 6 |
| 700 | 1 | _ | |a Syritsyn, Sergey |0 P:(DE-HGF)0 |b 7 |
| 773 | 1 | 8 | |a 10.1103/physrevd.99.114505 |b American Physical Society (APS) |d 2019-06-19 |n 11 |p 114505 |3 journal-article |2 Crossref |t Physical Review D |v 99 |y 2019 |x 2470-0010 |
| 773 | _ | _ | |a 10.1103/PhysRevD.99.114505 |g Vol. 99, no. 11, p. 114505 |0 PERI:(DE-600)2844732-3 |n 11 |p 114505 |t Physical review / D |v 99 |y 2019 |x 2470-0010 |
| 856 | 4 | _ | |u https://juser.fz-juelich.de/record/863701/files/PhysRevD.99.114505.pdf |y OpenAccess |
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