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Updated: May 4, 2026

Measurement of Coherence Decay in GaMnAs Using Femtosecond Four-wave Mixing
Published on: December 3, 2013
Modulation of the spin crossover behaviour in four manganese(III) complexes through cation-anion interactions
Suvamoy Malik1, Paula Brandão2, Samia Benmansour3
1Department of Chemistry, Jadavpur University, Kolkata-700032, India. amrita.saha@jadavpuruniversity.in.
Abstract:
Here we report the synthesis, structural and magnetic characterization of a series of manganese(III) monomers, formulated as [Mn(L)]X with X = PF6- (1), BF4- (2), I- (3) and Br-/NO3- (4). These four compounds have been prepared with a Schiff base ligand (HL) formed by the 2 : 1 condensation of an eugenol scaffold aldehyde and N,N'-bis(3-aminopropyl)ethylene-diamine. The structures of compounds 1-4 show in all cases the presence of the same [MnIII(L)]+ cation surrounded by different X- anions. Interestingly, the anions play a key role in determining not only the symmetry and cation-anion packing, which are quite different in compound 1 compared to those of compounds 2-4, but also the magnetic properties of the [MnIII(L)]+ cation. Variable temperature magnetic measurements show that in compound 1 the MnIII centre is in the high spin S = 2 state at any temperature, whereas compounds 2-4 show a smooth and incomplete spin crossover (SCO) from the low spin (S = 1) to the high spin (S = 2) ground state in the temperature range of 200-400 K. At 400 K the high spin fractions are around 31%, 27% and 42% for compounds 2-4, respectively. Isothermal magnetization measurements at low temperatures confirm the spin ground states in all cases. The magnetic data can be very well reproduced with a simple monomeric S = 2 (in 1) or S = 1 (in 2-4, for the low spin state) model with a zero-field splitting (ZFS) contribution (and a very weak intermolecular antiferromagnetic interaction in 2 and 4). Additionally, a detailed analysis of the structural parameters in compounds 2-4 shows that the Mn-N bond distances, the continuous shape parameters, the trigonal distortion angles (Φ) and the octahedral distortion parameters (Σ) show a significant increase when the temperature is increased from 100 to 398 K, confirming the presence of an incomplete SCO between 100 and 398 K in compounds 2-4.
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