Two series of copper-lanthanide heterometallic coordination polymers (CPs), [LnCu(2,3-pydc)(2)(suc)(0.5).H2O)(3)]center dot H2O [Ln = La (I), Pr (II), Nd (III), Sm (IV), Gd (V), and Eu (VI), 2,3-H(2)pydc = pyridine-2,3-dicarboxylic acid, H(2)suc = succinic acid], [Ln(2)Cu(3)(2,3-pydc)(6)(H2O)(10)]center dot 8H(2)O [Ln = Eu (VII), Tb (VIII), Dy (IX), and Er (X)], [Ln(2)Cu(2,3-pydc)(2)(suc)(mu(2)-OH)(2)(H2O)(2)]center dot 2H(2)O [Ln = Er (XI), Yb (XII), and Lu (XIII)], [Ln(2)Cu(2,3-pydc)(2)(suc)(2)(H2O)(6)]center dot 2H(2)O [Ln = Sm (1), Eu (2), Gd (3), Tb (4), Dy (5), and Er (6)], and Ln(2)Cu(2,3pydc) (2)(suc)(2)(H2O)(2) [Ln = Er (7), Yb (8), and Lu (9)], were successfully synthesized by the hydrothermal reactions of Cu.NO3)(2)center dot 3H(2)O, LnCl(3)center dot nH(2)O, 2,3-H(2)pydc, and H(2)suc. CPs 1-9 show two types of similar two-dimensional (2D) structures. In 1-9, the 2,3-pydc anions bridge the Cu-II ions into a one-dimensional (1D) loop chain, and the suc anions link the Ln(III) ions into a 1D double chain. The 1D loop chains and the 1D double chains connect each other to generate a 2D layer. The adjacent 2D layers are further packed into a three-dimensional (3D) supramolecular architecture by hydrogen-bonding interactions. CPs 4 and 6 display ferromagnetic interactions between the paramagnetic centers, and CP 5 shows a field-induced slow magnetic relaxation behavior. The structures and magnetic properties of I-XIII have been reported in previous work (Eur. J. Inorg. Chem., 2016, 1060).