The binary cyanide, Cu(CN) 2 , does not exist. However, copper(II) can be stabilised in a cyanide-only environment in the stoichiometric, mixed copper-nickel cyanide, CuNi(CN) 4 , and in the solid-solution, Cu 1-x Ni 1+x (CN) 4 (½ ≤ x < 1). The atomic structure of the layers in CuNi(CN) 4 and the stacking relationship between nearestneighbour layers have been determined from total neutron diffraction studies at 10 and 300 K. The structure consists of flat layers of perfectly square-planar [Ni(CN) 4 ] and [Cu(NC) 4 ] units linked by shared cyanide groups i.e. both the metal and cyanide groups are perfectly ordered with Cu(II) coordinated to the nitrogen end of the cyanide group and Ni(II) to the carbon end. The layered structure of this new mixed-metal cyanide is related to those of Ni(CN) 2 , which forms more extended sheets [1,2], and Pd(CN) 2 ·xNH 3 and Pt(CN) 2 ·xH 2 O, which form nanosheets [3]. The overall appearance of the powder X-ray diffraction pattern, including the unusual peak shapes of the observed Bragg reflections, has been successfully explained using models incorporating stacking disorder between next nearest neighbour layers. CuNi(CN) 4 shows similar thermal expansion behaviour to that observed previously for Ni(CN) 2 [1,4] with negative thermal expansion within the layers (α a = -9.7 MK -1 ) and positive thermal expansion between the layers (α c = +89 MK -1 ) measured over the temperature range 200-540 K.The stability of Cu(II) atoms in a cyanideonly environment has been investigated by varying the ratio of the Cu 2+ and Ni 2+ ions used in the synthesis. Using a Cu:Ni ratio of 1:1, the anhydrous phase, CuNi(CN) 4 , is precipitated directly. For Cu:Ni ratios less than one, hydrates of the form Cu 1-x Ni 1+x (CN) 4 ·yH 2 O (½ ≤ x < 1; y ≤ 6) are produced which can be dehydrated to form the corresponding anhydrous compounds, Cu 1-