“…K n (1) ,n (2) ,n (3) = 1) nor of the weight factor without explicitly referring to some gauge theory argument. However, from the algebraic viewpoint, besides the construction of the proposal being very simple and natural, we may observe that: i) thanks to the exponentiation {n (i) } Z n (1) ,n (2) ,n (3) ∼ exp( i S (i) ), when this operator is sandwiched between external Fock states with finite momentum (as necessary in order to have a pure defect partition function/Dotsenko-Fateev q-conformal block) the right number of screening charges is automatically picked up; also, the exponentiation hints to a worldsheet model similar to Liouville 2d CFT proposed in [59]; ii) the simple and specific weight factor may be needed once analytic, modular or crossing symmetry properties are imposed [35]; iii) the open questions may be solved by studying the more elementary Ding-Iohora-Miki algebra [81,82], the fundamental symmetry of matrix models arising in the present gauge theory context [83][84][85][86], which in our setup would give rise to the q-Virasoro algebra together with and additional Heisenberg algebra [87] which may play an important role here (similarly to the undeformed 4d case [88]). What we have discussed in this short note deserve further studies, also in view of a possible parallel story on S 4 which we leave for future work.…”