Insights to unusual antiferromagnetic behavior and exchange coupling interactions in Mn23C6

Abstract We report the structural, mechanical and electromagnetic properties of the intermetallic compound Mn 23 C 6 . The bulk Mn 23 C 6 sample was synthesized using high temperature high pressure quenching method (HTHPQM), and investigated in detail by x-ray diffraction, electron microscope, magnetization and electrical resistivity measurements, etc. First-principles calculation based on density functional theory ab intio simulation was carried out to calculate the bonding and electromagnetic properties of Mn 23 C 6 . Based on our experimental and simulated results, the Mn 23 C 6 in this work is single phase of a faced-centered cubic structure with space group Fm -3 m (No. 225). Determined by SEM and TEM, the bulk sample consists of monocrystal Mn 23 C 6 crystals with 2–15 μm grain sizes, it is the quick quenching method in the synthesizing process that brings such small crystal grain size. Archimedes method gives its density of 7.14 g/cm 3 , 95.74% of its theoretically calculated density 7.458 g/cm 3 . Owing to the abundant Mn 3d electrons and a framework of strongly linked Mn atoms in Mn 23 C 6 , the electrical conductivity is up to 8.47 × 10 −4 Ω⋅m, which shows that Mn 23 C 6 is a good conductor. Our magnetic susceptibility analyses reveal a magnetization peak in the M – T curve at 104 K, combined with the M – H curve and Curie–Weiss law, this peak usually means the transformation between paramagnetic and antiferromagnetic orders. To gain an insight into the mechanism of the magnetic phase transition, we calculated the magnetic properties, and the results show that different from normal antiferromagnetic order, the magnetic orders in Mn 23 C 6 consist of three parts, the direct ferromagnetic and antiferromagnetic exchange coupling interactions between Mn atoms, and the indirect antiferromagnetic super-exchange interaction between Mn and C atoms. Therefore, we reveal that the Mn 23 C 6 is a complex magnetic competition system including different magnetic orders and interactions, instead of the normal long-range antiferromagnetic order.