“…The latter have been worked out in [5,6]. This approach was applied to the nucleon electromagnetic form factors [7,8,9], where the second nucleon in the correlation function was interpolated with the three-quark current e.g., with the Ioffe current [10]. In order to access heavy baryons, e.g., Λ c or Λ b , one has to use a three-quark current with one heavy c or b quark.…”