GPa. Moreover, there is also a large kinetic barrier for diamond-graphite changes, in either direction. Even downhill spontaneous transformation from diamond to thermodynamically favored graphite (δg ≈ 20 meV/atom lower) is inhibited by a large barrier and would take geological times; good cause for a saying "diamonds are forever." [4] Nevertheless, at the nanoscale, such diamond graphitization [5,6] does occur through the outer atomic layers. This process can be suppressed by saturation of dangling sp 3 surface bonds with adatoms or covalent functional groups, for example, by hydrogenation, which "seals" the carbon in its energetically upper state, diamond. One could speculate that, conversely to graphitization, functionalizing the graphite surface can transform it to sp 3 state of diamond, to some depth; this however, is hindered by the energy taxing sp 3-sp 2 interface, created underneath. Moreover, although the 2D-surface can affect many properties of 3D bulk material, obviously the surface state (reconstruction or chemical passivation) cannot change the thermodynamics of phase preference across the entire macroscopic volume. High pressure, assisted by temperature, remains a prerequisite for getting 3D-diamonds from graphite. With the advent of 2D materials and particularly graphene (Gr), including its bilayer (BLG [7]) and few-layer (FLG [8]) varieties, this paradigm may change. In contrast to 3D bulk, if the sample is of very small, nanometer scale thickness, then its surface chemistry can switch the lattice organization (phase state) throughout. To appreciate the ease of such "phase conversion" by chemistry, one recalls best studied monolayer graphene hydrogenated on both sides into CH composition. It was theoretically proposed [9] and christened "graphane" in its detailed study. [10] Basic notable features distinguishing graphane are the sp 3-hybridizaton of all C-atoms (instead of sp 2 in graphene) and its wide band gap (5.4 eV in the graphane chair conformation, [11] instead of zero in semimetal graphene), which justify considering it as the ultimate, thinnest diamond slab [12] (especially since the bulk diamond surface is also typically H-passivated). The contrast in electronics of graphene and graphane invites possibilities of direct chemical patterning of functional circuitry. [13,14] The choice of active atoms is not limited to H, but can also be fluorine (interesting due to high chemical activity in its attachment to the graphene [13,15]), or chlorine. [16] The kinetics of such transformation was first analyzed in the context of hydrogen storage [17] and spillover [18] media, showing Nearly 2D diamond, or diamane, is coveted as an ultrathin sp 3-carbon film with unique mechanics and electro-optics. The very thinness (≈h) makes it possible for the surface chemistry, for example, adsorbed atoms, to shift the bulk phase thermodynamics in favor of diamond, from multilayer graphene. Thermodynamic theory coupled with atomistic first principles computations predicts not only the reduction of required pres...