The investigation of the tin-rich part of the ternary system Co/Ni/Sn yielded the phase Co(1)(-)(x)()Ni(x)()Sn(2) with the range of composition 0.23(3) < x < 0.59(3). When using a large excess of tin, Co(1)(-)(x)()Ni(x)()Sn(2) crystallizes at 500 degrees C in a structure isotypic to that of tetragonal PdSn(2) whereas a modification with the orthorhombic CoGe(2) structure type always forms from a stoichiometric mixture of the elemental components or from a tin melt at temperatures above 550 degrees C. The structures of Co(0.625)Ni(0.375)Sn(2) were determined by single-crystal X-ray diffraction methods (PdSn(2)-type space group I4(1)/acd, a = 6.2360(5) Å, c = 23.588(2) Å, Z = 16; CoGe(2)-type space group Aba2, a = 6.2439(4) Å, b = 6.2493(4) Å, c = 11.778(1) Å, Z = 8). Both structures have the same building unit consisting of three consecutive planar nets 4(4), 3(2)434, 4(4) formed by tin atoms. The condensation of the building blocks in the c direction gives rise to different stacking sequences. In the PdSn(2)-type, a ABCD sequence is realized and the c axis is doubled compared to the ideal CoGe(2)-type with AB stacking. Electron diffraction and high-resolution electron microscopy studies revealed the existence of other, complex, stacking variants as well as stacking faults in the Co(1)(-)(x)()Ni(x)()Sn(2) system.