Low-coordinate
metallic ions have been well recognized for constructing
good-performance single ion magnets (SIMs) due to their enhanced magnetic
anisotropy; however, the incorporation of such specific ions into
coordination polymers is still challenging. Here, we reported two
new Co<sup>II</sup> coordination polymers, namely [Co(pdms)(bpe)]<sub><i>n</i></sub> (<b>1</b>) and {[Co(pdms)(tpb)]·H<sub>2</sub>O·tpb}<sub><i>n</i></sub> (<b>2</b>)
(H<sub>2</sub>pdms = 1,2-bis(methanesulfonamido)benzene, bpe = 1,2-di(4-pyridyl)ethane,
tpb = 1,2,4,5-tetra(4-pyridyl)benzene). Single crystal X-ray diffraction
experiments indicated that the Co<sup>II</sup> centers in both <b>1</b> and <b>2</b> display a distorted tetrahedral geometry
with quasi <i>C</i><sub>2<i>v</i></sub> symmetry
and are linked into a one-dimensional (1D) <i>zig</i>-<i>zag</i> chain via the ditopic bridging ligand of bpe in <b>1</b> while a ribbon chain via the tetradentate linker of tpb
in <b>2</b>. Magnetic studies revealed the easy-axis magnetic
anisotropy of the Co<sup>II</sup> ions with different zero-field splitting <i>D</i> of −19 cm<sup>–1</sup> (<b>1</b>)
and −33 cm<sup>–1</sup> (<b>2</b>), likely due
to the distinct changes in the N<sub>py</sub>–Co–N<sub>py</sub> bite angles (100.20° (<b>1</b>) vs. 93.90°
(<b>2</b>)). Moreover, slow magnetic relaxation proceeded via
different relaxation mechanisms under applied dc fields was observed,
giving an effective energy barrier (<i>U</i><sub>eff</sub>) of 69.6 K for <b>1</b> and 76.6 K for <b>2</b>, respectively.
The <i>ab initio</i> calculations on both the polymers further
confirmed the sign and magnitude of the ZFS parameters and nicely
reproduced the experimental results. Our study demonstrated a great
potential for applying the well-studied and highly anisotropic 4-coordinate
metal ions within a coordination polymer, opening a viable means to
tuning magnetic anisotropy via topological control.