Abstract:Two new dinuclear iron(II) complexes (1·PF 6 and 1·AsF 6 ) of the general formula [Fe II 2 (L2 C3 ) 2 ](X) 4 ·nH 2 O·mMeCN (X = PF 6 , n = m = 1.5 for 1·PF 6 and X = AsF 6 , n = 3, m = 1 for 1·AsF 6 ) have been prepared and structurally characterized, where L2 C3 is a bis-1,2,3-triazolimine type Schiff-baseSingle crystal X-ray structure analyses revealed that 1·PF 6 and 1·AsF 6 are isostructural. The complex-cation [Fe II 2 (L2 C3 ) 2 ] 4+ of both has the same dinuclear double helicate architecture, in which each iron(II) center has an N6 octahedral coordination environment. Neighboring helicates are connected by intermolecular π-π interactions to give a chiral one-dimensional (1D) structure, and cationic 1D chains with the opposite chirality exist in the crystal lattice to give a heterochiral crystal. Magnetic and differential scanning calorimetry (DSC) studies were performed only for 1·AsF 6 , since the thermal stability in a high-temperature spin crossover (SCO) region of 1·PF 6 is poorer than that of 1·AsF 6 . 1·AsF 6 shows an unsymmetrical hysteretic SCO between the low-spin-low-spin (LS-LS) and high-spin-high-spin (HS-HS) states at above room temperature. The critical temperatures of warming (T c ↑) and cooling (T c ↓) modes in the abrupt spin transition area are 485 and 401 K, respectively, indicating the occurrence of 84 K-wide thermal hysteresis in the first thermal cycle.