Abstract
We summarize our results for hadronic contributions to the anomalous magnetic moment of the muon (), the one from hadronic vacuum-polarisation (HVP) and the light-by-light scattering contribution (LBL), obtained from the Dyson-Schwinger equations (DSE's) of QCD. In the case of HVP we find good agreement with model independent determinations from dispersion relations for as well as for the Adler function with deviations well below the ten percent level. From this we conclude that the DSE approach should be capable of describing with similar accuracy. We also present results for LBL using a resonance expansion of the quark anti-quark T-matrix. Our preliminary value is .
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