A new and detailed measurement of the cross section for hard exclusive neutral-pion muoproduction on the proton was performed in a wide kinematic region, with the photon virtuality Q2 ranging from 1 to 8 (GeV/ c)2 and the Bjorken variable xBj ranging from 0.02 to 0.45. The data were collected at COMPASS at CERN using 160 GeV/ c longitudinally polarised μ+ and μ− beams scattering off a 2.5 m long liquid hydrogen target. From the average of the measured μ+ and μ− cross sections, the virtual-photon–proton cross section is determined as a function of the squared four-momentum transfer between the initial and final state proton in the range 0.08 (GeV/ c)2 <|t|< 0.64 (GeV/ c)2 . From its angular distribution, the combined contribution of transversely and longitudinally polarised photons are determined, as well as transverse–transverse and longitudinal–transverse interference contributions. They are studied as functions of four-momentum transfer |t| , photon virtuality Q2 and virtual-photon energy ν . The longitudinal–transverse interference contribution is found to be compatible with zero. The significant transverse–transverse interference contribution reveals the existence of a dominant contribution by transversely polarised photons. This could provide clear experimental evidence for the chiral-odd GPD E‾T . In addition, the existence of a non-negligible contribution of longitudinally polarised photons is suggested by the |t| -dependence of the cross section at xBj< 0.1. Altogether, these results provide valuable input for future modelling of GPDs and thus of cross sections for exclusive pseudo-scalar meson production. Furthermore, they can be expected to facilitate the study of next-to-leading order corrections and higher-twist contributions.
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Alexeev et al. (2025) studied this question.
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