The 1 D2 charmonium assignment for the X(3872) meson is considered, as prompted by a recent result from the BABAR Collaboration, favouring 2 −+ quantum numbers for the X. It is shown that established properties of the X(3872) are in a drastic conflict with the 1 D2 cc assignment. PACS numbers: 14.40.Pq, 13.25.Gv, 12.39.Pn Seven years after its discovery, the X(3872) meson has confirmed once again its reputation of enfante terrible of meson spectroscopy. The state was first seen by Belle [1] in the π + π − J/ψ mode and then confirmed, in the same discovery mode, by the CDF [2], D∅ [3], and BABAR [4] Collaborations. According to the CDF analysis of the dipion mass spectrum and the angular distribution in the π + π − J/ψ mode [5], only 1 ++ and 2 −+ assignments are able to describe the data. Then, while the nature of the state remains controversial, there are good phenomenological reasons to assign it 1 ++ quantum numbers.First, the X resides at the D 0D * 0 threshold, which prompts a considerable admixture of a molecule in its wave function. Furthermore, CDF concludes that the π + π − come from the ρ [6] which, together with the Belle observation of the ωJ/ψ mode [7], points to a considerable isospin violation. The latter can be explained naturally in the molecular model of the X, which implies 1 ++ quantum numbers. In addition, the X was also observed in the D 0D * 0 mode with a significant rate [8][9][10]. Both ρJ/ψ and D 0D * 0 modes were analysed simultaneously in Refs. [11][12][13], and it was shown that indeed the data were compatible with a large admixture of the D 0D * 0 molecular component in the wave function of the X.However, a recent analysis of the decay B → KωJ/ψ data performed by the BABAR Collaboration [14] indicates that inclusion of an extra unit of the orbital angular momentum in the ωJ/ψ system improves significantly the overall description of the observed π + π − π 0 mass distribution, which implies a negative P -parity of the X(3872) state. Although this new BABAR result is fully compatible with the 2 −+ assignment allowed by CDF, if confirmed, it clearly challenges our understanding of the charmonium spectroscopy above the open-charm threshold. Here we investigate the most conventional explanation for the 2 −+ X(3872) as the 1 1 D 2 charmonium state.In case of charmonium D-levels we have an experimental anchor at our disposal -the ψ(3770) vector state which is dominantly a cc state, with the angular momentum of the quark-antiquark pair L = 2 and the total quark spin S = 1 ( 1 D 2 state has L = 2 and S = 0). As c-quark is heavy, the spin-orbit force, which splits spin-triplet and spin-singlet levels, is not large and all D-levels are degenerate in the leading-order approximation. Hence, one may use the data on the 3 D 1 level to estimate the mass and matrix elements of the 1 D 2 level.