“… 13 , 14 In order to maximize the MCE, weak superexchange interactions in materials having high density of magnetic centres are highly desired; along this front the use of geometric spin frustration, like 2D triangular AF lattices, gives rise to regions of high density of states. 15 Thus, the highly dense, almost hexagonal, 2D lattice of lanthanide cations bridged by hydroxide ligands present in LLHs, together with its low diamagnetic content, is a promising alternative to the list of extended materials with short bridges reported so far with MCE, which includes, among others, formates, 16 , 17 phosphates 18 and carbonates, 19 being [Gd(HCOO)(OAc) 2 (H 2 O) 2 ], 20 [Gd(C 4 O 4 )(OH)(H 2 O) 4 ] n , 21 [Gd(C 2 O 4 )(H 2 O) 3 Cl], 22 and [Gd(cit)(H 2 O)], 23 the only 2D structures. Importantly, the ability of LLHs to be delaminated 3 provides additional advantages for rapid heat dissipation, as the delaminated material could be placed on a substrate thus enhancing heat transportation.…”