Abstract

We report a lattice QCD determination of the πγ→πππγ\to ππ transition amplitude for the PP-wave, I=1I=1 two-pion final state, as a function of the photon virtuality and ππππ invariant mass. The calculation was performed with 2+12+1 flavors of clover fermions at a pion mass of approximately 320320 MeV, on a 323×9632^3 \times 96 lattice with L≈3.6L\approx 3.6 fm. We construct the necessary correlation functions using a combination of smeared forward, sequential and stochastic propagators, and determine the finite-volume matrix elements for all ππππ momenta up to ∣P⃗∣=32πL|\vec{P}|= \sqrt{3} \frac{2π}{L} and all associated irreducible representations. In the mapping of the finite-volume to infinite-volume matrix elements using the Lellouch-Lüscher factor, we consider two different parametrizations of the ππππ scattering phase shift. We fit the q2q^2 and ss dependence of the infinite-volume transition amplitude in a model-independent way using series expansions, and compare multiple different truncations of this series. Through analytic continuation to the ρρ resonance pole, we also determine the πγ→ρπγ\to ρ resonant transition form factor and the ρρ meson photocoupling, and obtain ∣Gρπγ∣=0.0802(32)(20)|G_{ρπγ}| = 0.0802(32)(20).

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