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.