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Coordination polymers containing dicyanamide (N(CN)
2
−, dca) or tricyanomethanide (C(CN)
3
−, tcm) bridging ligands are described from the perspective of their structure and magnetism. The binary compounds α-M(dca)
2 form an isostructural series (M=Cr, Mn, Fe, Co, Ni, Cu) having a single rutile-like network that involves μ
1,3,5-dca bridging. They display quite diverse types of long-range magnetic order viz. canted-spin antiferromagnets (Cr, Mn, Fe), ferromagnets (Co, Ni, Cu). An up-to-date review is given of the diverse range of physical measurements made on the α-M(dca)
2 series together with interpretations for the different net exchange coupling and consequent 3D order. The doubly interpenetrating rutile network M(tcm)
2 series generally do not show long-range order except for a few members at very low temperatures. The ‘mixed’ self-penetrating network compounds M(dca)(tcm) do show long-range order (M=Co, Ni), albeit at lower
T
c values than for the M(dca)
2 parents. Modification of the M–dca networks is possible by incorporation of coligands into the structures. Ternary species of type M(dca)
2(L)
n
, where L is a terminal (e.g. pyridine, MeOH) or a bridging (e.g. pyrazine, 4,4′-bipyridine) coligand, display a diverse range of 1D, 2D and 3D structural types. With a few exceptions, the large number of compounds structurally characterised contain μ
1,5-dca bridging and display very weak antiferromagnetic coupling (
J<ca. −1 cm
−1), typical of this bridging mode. Compounds such as Mn(dca)
2(pyrazine) display a magnetic phase transition at low temperatures. This is also the case in the isostructural 2D layer compounds M(dca)
2(H
2O) · phenazine (M=Fe, Ni) which, perhaps not surprisingly, do not have coordinated phenazines but, rather, phenazines intercalated between layers of M(dca)
2(H
2O) in which μ
1,3,5 and μ
1,5-dca bridging exists. Anionic networks of types M(dca)
3
− and M(dca)
4
2− formed by templation around cations of the organic (e.g. Ph
4E
+, R
4N
+) or inorganic (M(2,2′-bipyridine)
3
2+) types are described. The latter display no magnetic interactions between the weakly antiferromagnetically coupled anionic sub-lattice and the paramagnetic cationic sub-lattice.