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088 | 1 | _ | |a arXiv:1909.10744 |
088 | _ | _ | |a arXiv:1909.10744 |2 arXiv |
100 | 1 | _ | |a Alexandrou, C. |0 P:(DE-HGF)0 |b 0 |
245 | _ | _ | |a Nucleon strange electromagnetic form factors |
260 | _ | _ | |a Melville, NY |c 2020 |b Inst.302363 |
264 | _ | 1 | |3 online |2 Crossref |b American Physical Society (APS) |c 2020-02-13 |
264 | _ | 1 | |3 print |2 Crossref |b American Physical Society (APS) |c 2020-02-01 |
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336 | 7 | _ | |a ARTICLE |2 BibTeX |
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336 | 7 | _ | |a Journal Article |0 0 |2 EndNote |
500 | _ | _ | |a 7 pages and 5 figures ; publication: Phys.Rev. D101 3 (2020) 031501 ; ; |
520 | _ | _ | |a The role of the strange quarks on the low-energy interactions of the proton can be probed through the strange electromagnetic form factors. Knowledge of these form factors provides essential input for parity-violating processes and contributes to the understanding of the sea quark dynamics. We determine the strange electromagnetic form factors of the nucleon within the lattice formulation of Quantum Chromodynamics using simulations that include light, strange and charm quarks in the sea all tuned to their physical mass values. We employ state-of-the-art techniques to accurately extract the form factors for values of the momentum transfer square up to 0.8~GeV$^2$. We find that both the electric and magnetic form factors are statistically non-zero. We obtain for the strange magnetic moment $\mu^s=-0.017(4)$, the strange magnetic radius $\langle r^2_M \rangle^s=-0.015(9)$~fm$^2$, and the strange charge radius $\langle r^2_E \rangle^s=-0.0048(6)$~fm$^2$. |
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542 | _ | _ | |i 2020-02-13 |2 Crossref |u https://creativecommons.org/licenses/by/4.0/ |
588 | _ | _ | |a Dataset connected to CrossRef |
650 | _ | 7 | |a form factor: electromagnetic |2 autogen |
650 | _ | 7 | |a form factor: magnetic |2 autogen |
650 | _ | 7 | |a nucleon: form factor: electromagnetic |2 autogen |
650 | _ | 7 | |a quark: sea |2 autogen |
650 | _ | 7 | |a p: interaction |2 autogen |
650 | _ | 7 | |a quantum chromodynamics |2 autogen |
650 | _ | 7 | |a momentum transfer |2 autogen |
650 | _ | 7 | |a magnetic moment |2 autogen |
650 | _ | 7 | |a charge radius |2 autogen |
650 | _ | 7 | |a lattice |2 autogen |
650 | _ | 7 | |a charm |2 autogen |
693 | _ | _ | |0 EXP:(DE-MLZ)NOSPEC-20140101 |5 EXP:(DE-MLZ)NOSPEC-20140101 |e No specific instrument |x 0 |
700 | 1 | _ | |a Bacchio, S. |b 1 |
700 | 1 | _ | |a Constantinou, M. |b 2 |
700 | 1 | _ | |a Finkenrath, J. |b 3 |
700 | 1 | _ | |a Hadjiyiannakou, K. |b 4 |
700 | 1 | _ | |a Jansen, Karl |0 P:(DE-H253)PIP1003636 |b 5 |
700 | 1 | _ | |a Koutsou, G. |b 6 |
773 | 1 | 8 | |a 10.1103/physrevd.101.031501 |b American Physical Society (APS) |d 2020-02-13 |n 3 |p 031501 |3 journal-article |2 Crossref |t Physical Review D |v 101 |y 2020 |x 2470-0010 |
773 | _ | _ | |a 10.1103/PhysRevD.101.031501 |g Vol. 101, no. 3, p. 031501 |0 PERI:(DE-600)2844732-3 |n 3 |p 031501 |t Physical review / D |v 101 |y 2020 |x 2470-0010 |
787 | 0 | _ | |a Alexandrou, C. et.al. |0 PUBDB-2020-00048 |t Nucleon strange electromagnetic form factors |i IsMemberOf |d 2019 |
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914 | 1 | _ | |y 2020 |
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