Boussarie, R.
Pire, B.
Szymanowski, L.
Wallon, S.
Article History
Received: 14 September 2016
Revised: 15 December 2016
Accepted: 17 January 2017
First Online: 9 February 2017
Change Date: 4 October 2018
Change Type: Erratum
Change Date: 4 October 2018
Change Type: Erratum
Change Type: Erratum
Change Details: An unfortunate misprint in our numerical code has led to an overestimate of the cross section for the exclusive photoproduction of a ? ?L pair in the kinematics where the pair has a large invariant mass and the final nucleon has a small transverse momentum, described in the collinear factorization framework. The rates are thus expected to be smaller but the possibility to disentangle the transversity GPDs through the process where the ??meson is transversely polarized is enhanced.
Change Details: An unfortunate misprint in our numerical code has led to an overestimate of the cross section for the exclusive photoproduction of a ? ?L pair in the kinematics where the pair has a large invariant mass and the final nucleon has a small transverse momentum, described in the collinear factorization framework. The rates are thus expected to be smaller but the possibility to disentangle the transversity GPDs through the process where the ??meson is transversely polarized is enhanced.
Change Date: 4 October 2018
Change Details: An unfortunate misprint in our numerical code has led to an overestimate of the cross section for the exclusive photoproduction of a ? ?L pair in the kinematics where the pair has a large invariant mass and the final nucleon has a small transverse momentum, described in the collinear factorization framework. The rates are thus expected to be smaller but the possibility to disentangle the transversity GPDs through the process where the ??meson is transversely polarized is enhanced.