Journal
PHYSICAL REVIEW LETTERS
Volume 118, Issue 23, Pages -Publisher
AMER PHYSICAL SOC
DOI: 10.1103/PhysRevLett.118.232001
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Funding
- DFG [SFB/TR 16, SFB/TR 110]
- DOE [DE-FG02-00ER41132]
- National Science Foundation [NSF PHY-1125915]
- Marie Curie Intra-European Fellowship of the European Community's 7th Framework Programme [PIEF-GA-2013-622527]
- Swiss National Science Foundation [P300P2_167751]
- Swiss National Science Foundation (SNF) [P300P2_167751] Funding Source: Swiss National Science Foundation (SNF)
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We present a first model-independent calculation of pp intermediate states in the hadronic-light-by-light (HLBL) contribution to the anomalous magnetic moment of the muon (g -2)(mu) that goes beyond the scalar QED pion loop. To this end, we combine a recently developed dispersive description of the HLBL tensor with a partial-wave expansion and demonstrate that the known scalar-QED result is recovered after partial-wave resummation. Using dispersive fits to high-statistics data for the pion vector form factor, we provide an evaluation of the full pion box ap box a(mu)(pi box) = -15.9(2) x 10(-11). We then construct a suitable input for the gamma*gamma* -> pi pi helicity partial waves, based on a pion-pole left-hand cut and show that for the dominant charged-pion contribution, this representation is consistent with the two-loop chiral prediction and the COMPASS measurement for the pion polarizability. This allows us to reliably estimate S-wave rescattering effects to the full pion box and leads to our final estimate for the sum of these two contributions a(mu)(pi box) + a(mu,J=0)(pi pi,pi-pole) (LHC) = -24(1) x 10(-11).
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