“…For fully differential exclusive cross sections, QCD corrections to the second order (next-to-next-to-leading order, NNLO) were computed for the 2 → 1 processes vectorboson production [6,7] and Higgs-boson production [8,9] already about a decade ago. In recent years, NNLO calculations have become available for many 2 → 2 reactions at hadron colliders: pp → γγ [10], pp → V H [11], pp → V γ [12], pp → tt [13,14], pp → H+j [15,16], pp → W + j [17,18], pp → Z + j [19,20], pp → γ + X [21], pp → ZZ [22], pp → WW [23], pp → ZW [24] and pp → 2j [25], as well as for the electron-positron collisions e + e − → 3j [26,27] and lepton-proton processes ep → 1j [28] ep → 2j [29] and for the related 2 → 3 hadron-collider process of Higgs production in vector boson fusion [30,31]. These NNLO calculations of fully differential exclusive cross sections were enabled by substantial methodological developments [31][32][33][34][35][36][37][38] of infrared subtraction methods for the handling of singular contributions that appear in all parton-level subprocesses.…”