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001 | 474786 | ||
005 | 20250715175927.0 | ||
024 | 7 | _ | |a 10.22323/1.396.0519 |2 doi |
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024 | 7 | _ | |a inspire:1985868 |2 inspire |
024 | 7 | _ | |a arXiv:2112.03586 |2 arXiv |
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088 | _ | _ | |a arXiv:2112.03586 |2 arXiv |
100 | 1 | _ | |a Burri, Sebastian Andreas |0 S.Burri.1 |b 0 |e Corresponding author |
111 | 2 | _ | |a The 38th International Symposium on Lattice Field Theory |g Lattice 2021 |c Zoom/Gather@Massachusetts Institute of Technology |d 2021-07-26 - 2021-07-30 |w USA |
245 | _ | _ | |a Pion-pole contribution to HLbL from twisted mass lattice QCD at the physical point |
260 | _ | _ | |a Trieste |c 2022 |b SISSA |
300 | _ | _ | |a 9 |
336 | 7 | _ | |a CONFERENCE_PAPER |2 ORCID |
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490 | 0 | _ | |a 1985868 |2 Author |
500 | _ | _ | |a 9 pages, 7 figures; Proceedings of the 38th International Symposium on Lattice Field Theory - Lattice 2021, Zoom/Gather@Massachusetts Institute of Technology |
520 | _ | _ | |a We report on our computation of the pion transition form factor ${\cal F}_{P\rightarrow \gamma^*\gamma^*}$ from twisted mass lattice QCD in order to determine the numerically dominant light pseudoscalar pole contribution in the hadronic light-by-light scattering contribution to the anomalous magnetic moment of the muon $a_\mu =(g-2)_\mu$. The pion transition form factor is computed directly at the physical point. We present first results for our estimate of the pion-pole contribution with kinematic setup for the pion at rest. |
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650 | _ | 7 | |a mass: twist |2 INSPIRE |
650 | _ | 7 | |a form factor: transition |2 INSPIRE |
650 | _ | 7 | |a muon: magnetic moment |2 INSPIRE |
650 | _ | 7 | |a photon photon: scattering |2 INSPIRE |
650 | _ | 7 | |a lattice field theory |2 INSPIRE |
650 | _ | 7 | |a kinematics |2 INSPIRE |
650 | _ | 7 | |a pole |2 INSPIRE |
650 | _ | 7 | |a at rest |2 INSPIRE |
650 | _ | 7 | |a pseudoscalar |2 INSPIRE |
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700 | 1 | _ | |a Alexandrou, Constantia |b 1 |
700 | 1 | _ | |a Bacchio, Simone |0 S.Bacchio.1 |b 2 |
700 | 1 | _ | |a Bergner, Georg |0 G.Bergner.1 |b 3 |
700 | 1 | _ | |a Finkenrath, Jacob |b 4 |
700 | 1 | _ | |a Gasbarro, Andrew |0 A.D.Gasbarro.1 |b 5 |
700 | 1 | _ | |a Hadjiyiannakou, Kyriakos |0 K.Hadjiyiannakou.5 |b 6 |
700 | 1 | _ | |a Jansen, Karl |0 P:(DE-H253)PIP1003636 |b 7 |
700 | 1 | _ | |a Kostrzewa, Bartosz |0 P:(DE-H253)PIP1014927 |b 8 |
700 | 1 | _ | |a Koutsou, Giannis |b 9 |
700 | 1 | _ | |a Ottnad, Konstantin |b 10 |
700 | 1 | _ | |a Petschlies, Marcus |b 11 |
700 | 1 | _ | |a Pittler, Ferenc |0 F.Pittler.1 |b 12 |
700 | 1 | _ | |a Steffens, Fernanda |0 P:(DE-H253)PIP1020874 |b 13 |
700 | 1 | _ | |a Urbach, Carsten |b 14 |
700 | 1 | _ | |a Wenger, Urs |0 U.Wenger.1 |b 15 |
773 | _ | _ | |a 10.22323/1.396.0519 |0 PERI:(DE-600)2642026-0 |p 519 |t Proceedings of Science / International School for Advanced Studies |v (LATTICE2021) |y 2022 |x 1824-8039 |
787 | 0 | _ | |a Burri, Sebastian Andreas et.al. |d 2022 |i IsParent |0 PUBDB-2022-06924 |r arXiv:2112.03586 |t Pion-pole contribution to HLbL from twisted mass lattice QCD at the physical point |
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