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Rescattering effects in the hadronic-light-by-light contribution to the anomalous magnetic moment of the muon
We present a first model-independent calculation of ππ intermediate states in the hadronic-light-by-light (HLBL) contribution to the anomalous magnetic moment of the muon (g-2)μ that goes beyond the scalar QED pion loop. To this end, we combine a recently developed dispersive description of the HLBL...
Autores principales: | , , , |
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Lenguaje: | eng |
Publicado: |
2017
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1103/PhysRevLett.118.232001 http://cds.cern.ch/record/2243468 |
Sumario: | We present a first model-independent calculation of ππ intermediate states in the hadronic-light-by-light (HLBL) contribution to the anomalous magnetic moment of the muon (g-2)μ 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 aμπ box=-15.9(2)×10-11. We then construct a suitable input for the γ*γ*→ππ 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 aμπ box+aμ,J=0ππ,π-pole LHC=-24(1)×10-11. |
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