Paramagnetic molecular materials with electronic structures sensitive to the environment are very attractive owing to potential applications in molecular devices and sensors. [1] Great efforts have been made in synthesizing bistable paramagnetic molecules or polymers that exist in two different spin states, which can be tuned by an external stimulus such as temperature, pressure, or light. [2][3][4] Cobalt ions can exist in multiple oxidation states, and hence are good candidates for construction of molecular materials that can switch between two different oxidation states, typically between Co III and Co
II. A number of cobalt semiquinonate complexes undergo valence transition in response to external stimuli such as temperature and light (valence tautomerism). [5,6] In a few bimetallic compounds, such as Co-Fe(Os) cyanometalates, thermally induced charge transfer occurs between the two redox-active metal ions. [7] The shift of the equilibrium between Co III and Co II is accompanied by a drastic change in their magnetic and optical properties. As far as we are aware, valence changes in cobalt coordination polymers induced by a second metal coordination sphere have never been described in the literature.Here we present a novel approach to manipulate the oxidation state of cobalt by a controllable second metal coordination sphere. Polytopic ligand 1,4,7-triazacyclononane-1,4,7-triyl-tris(methylenephosphonic acid) ( Compound 1 a is a rare example of metal phosphonates with both 3d and 4f metal ions.[8] It crystallizes in monoclinic space group P2 1 /c.[9] The octahedral Co III ion is surrounded by three phosphonate oxygen atoms (O2, O5, and O8) and three nitrogen atoms (N1, N2, and N3) from the same notp 6À ligand in a mononuclear Co (4) ). This unit behaves as a tetradentate "ligand" and links to four La III ions through phosphonate oxygen atoms O1, O3, O4, and O7 to form a two-dimensional waved layer containing six-and eight-membered rings. Each La atom is coordinated by eight oxygen atoms, four of which are phosphonate oxygen atoms from four Co(notp) 3À units, and the remainder oxygen atoms of water molecules. The interlayer space is filled by the lattice water molecules with extensive hydrogen-bonding interactions (Figure 1 a and b). Thermal analysis and XRD measurements confirm that both the coordinated and lattice water molecules can be removed on heating to 220 8C with retention of the network structure. The fully dehydrated sample H[hs-Co II La III (notp)] (1 a-220) can be redissolved in water, from which crystalline 1 a can be obtained within one day in the presence of oxygen (Supporting Information).Magnetic susceptibilities, measured in the temperature range 1.8-300 K under an external field of 2 kOe (Figure 1 c), reveal a diamagnetic nature for compound 1 a, in agreement with the presence of a low-spin Co III (m eff /Co(300 K) = 0 m B ). After heating 1 a at 120 8C for 1 h, the resulting sample 1 a-120 becomes paramagnetic. The paramagnetic behavior becomes more significant if 1 a is heated at a higher ...