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Measurement of the Quantum Tunneling Gap in a Dysprosocenium Single-Molecule Magnet
[Image: see text] We perform magnetization sweeps on the high-performing single-molecule magnet [Dy(Cp(ttt))(2)][B(C(6)F(5))(4)] (Cp(ttt) = C(5)H(2)(t)Bu(3)-1,2,4; (t)Bu = C(CH(3))(3)) to determine the quantum tunneling gap of the ground-state avoided crossing at zero-field, finding a value on the o...
Autores principales: | , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical Society
2023
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9986949/ https://www.ncbi.nlm.nih.gov/pubmed/36812166 http://dx.doi.org/10.1021/acs.jpclett.3c00034 |
Sumario: | [Image: see text] We perform magnetization sweeps on the high-performing single-molecule magnet [Dy(Cp(ttt))(2)][B(C(6)F(5))(4)] (Cp(ttt) = C(5)H(2)(t)Bu(3)-1,2,4; (t)Bu = C(CH(3))(3)) to determine the quantum tunneling gap of the ground-state avoided crossing at zero-field, finding a value on the order of 10(–7) cm(–1). In addition to the pure crystalline material, we also measure the tunnel splitting of [Dy(Cp(ttt))(2)][B(C(6)F(5))(4)] dissolved in dichloromethane (DCM) and 1,2-difluorobenzene (DFB). We find that concentrations of 200 or 100 mM [Dy(Cp(ttt))(2)][B(C(6)F(5))(4)] in these solvents increases the size of the tunneling gap compared to the pure sample, despite a similarity in the strength of the dipolar fields, indicating that either a structural or vibrational change due to the environment increases quantum tunneling rates. |
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