“…Theorem A follows from Theorem B by choosing l such that L(1/2, g ⊗ χ l ) = 0 and letting f γ = ϑ l,χ (ϕ g ) (see Section 6 for the details). The proof of Theorem B relies on our previous articles [ST18,ST20], which made strong restrictions on the functions γ, as well as on the weight and on the signs ε g (v), that we now lift. It is based on the results from [Zha01,Xue06] giving central values in terms of height parings, which we relate to Fourier coefficients.…”