Metal–organic
frameworks (MOFs) provide exceptional chemical
tunability and have recently been demonstrated to exhibit electrical
conductivity and related functional electronic properties. The kagomé
lattice is a fruitful source of novel physical states of matter, including
the quantum spin liquid (in insulators) and Dirac fermions (in metals).
Small-bandgap kagomé materials have the potential to bridge
quantum spin liquid states and exhibit phenomena such as superconductivity
but remain exceptionally rare. Here we report a structural, thermodynamic,
and transport study of the two-dimensional kagomé metal–organic
frameworks Ni3(HIB)2 and Cu3(HIB)2 (HIB = hexaiminobenzene). Magnetization measurements yield
Curie constants of 0.989 emu K (mol Ni)−1 Oe–1 and 0.371 emu K (mol Cu)−1 Oe–1, respectively, close to the values expected for ideal S = 1 Ni2+ and S = 1/2 Cu2+. Weiss temperatures of −10.6
and −14.3 K indicate net weak mean field antiferromagnetic
interactions between ions. Electrical transport measurements reveal
that both materials are semiconducting, with gaps (E
g) of 22.2 and 103 meV, respectively. Specific heat measurements
reveal a large T-linear contribution γ of 148(4)
mJ mol-fu–1 K–2 in Ni3(HIB)2 with only a gradual upturn below ∼5 K and
no evidence of a phase transition to an ordered state down to 0.1
K. Cu3(HIB)2 also lacks evidence of a phase
transition above 0.1 K, with a substantial, field-dependent, magnetic
contribution below ∼5 K. Despite them being superficially in
agreement with the expectations of magnetic frustration and spin liquid
physics, we ascribe these observations to the stacking faults found
from a detailed analysis of synchrotron X-ray diffraction data. At
the same time, our results demonstrate that these MOFs exhibit localized
magnetism with simultaneous proximity to a metallic state, thus opening
up opportunities to explore the connection between the insulating
and metallic ground states of kagomé materials in a highly
tunable chemical platform.