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Updated: May 15, 2026

Light-driven Molecular Motors on Surfaces for Single Molecular Imaging
Published on: March 13, 2019
Single molecule magnets with m-fluorobenzoate and difluoromethylacetate as polar ligands
Norihisa Hoshino1, Takuya Shiga, Hiroki Oshio
1Institute of Multidisciplinary Research for Advanced Materials (IMRAM), Tohoku University, 2-1-1 Katahira, Sendai 980-8577, Japan. hoshino@tagen.tohoku.ac.jp
Abstract:
Two new single molecule magnets (SMMs), [Mn(12)O(12)(CHF(2)COO)(16)(H(2)O)(4)]·2CH(2)Cl(2)·4H(2)O (1) and [Mn(12)O(12)(m-FPhCOO)(16)(H(2)O)(4)]·2(m-FPhCOOH)·7CH(2)Cl(2) (2), based on a disc-shaped {Mn(12)O(12)}-framework with difluoromethylacetate (CHF(2)COO(-)) and m-fluorobenzoate (m-FPhCOO(-)) as polar ligands were prepared in CH(2)Cl(2). Structural analyses by X-ray diffraction at 100 K showed orientationally disordered fluorine atoms in the CHF(2)COO(-) and m-FPhCOO(-) ligands of crystals 1 and 2, respectively. In crystal 1, the fluorine atoms at the axial coordination sites of the disc-like {Mn(12)O(12)}-framework exhibited large thermal parameters even at 100 K, suggesting that thermally activated rotation of the -CHF(2) groups along the C-COO axis occurred in the CHF(2)COO(-) ligands. The SMMs behaviors of crystals 1 and 2 showed magnetization hysteresis at 1.8 K and frequency-dependent in-phase and out-of-phase ac magnetic susceptibilities, characteristic of SMMs. Frequency-dependent dielectric responses as well as two Debye-type relaxation processes at ~100 and ~220 K were observed in crystal 1, while such responses were not observed in crystal 2. The activation energy and blocking temperature of the relaxation process for 1 were 12 kJ mol(-1) and 48 K, respectively, at ~100 K, whereas those at ~220 K were 66 kJ mol(-1) and 153 K, respectively. In 1 , the two polarization types at ~100 and ~220 K were associated with thermally activated fluctuations of the hydrogen-bonded crystalline H(2)O molecules and rotation of the -CHF(2) group in the CHF(2)COO(-) ligand.
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When atoms or molecules absorb light at the proper frequency, their electrons are excited to higher-energy orbitals. For many main group atoms and molecules, the absorbed photons are in the ultraviolet range of the electromagnetic spectrum, which cannot be detected by the human eye. For coordination compounds, the energy difference between the d orbitals often allows photons in the visible range to be absorbed and emitted, which is seen as colors by the human eye.
