Abstract

We present preliminary results on the axial form factor GA(Q2)G_A(Q^2) and the induced pseudoscalar form factor GP(Q2)G_P(Q^2) of the nucleon. A systematic analysis of the excited-state contributions to form factors is performed on the CLS ensemble `N6' with mπ=340 MeVm_π= 340 \ \text{MeV} and lattice spacing a∼0.05 fma \sim 0.05 \ \text{fm}. The relevant three-point functions were computed with source-sink separations ranging from ts∼0.6 fmt_s \sim 0.6 \ \text{fm} to ts∼ 1.4 fmt_s \sim \ 1.4 \ \text{fm}. We observe that the form factors suffer from non-trivial excited-state contributions at the source-sink separations available to us. It is noted that naive plateau fits underestimate the excited-state contributions and that the method of summed operator insertions correctly accounts for these effects.

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