2021
DOI: 10.1021/acs.inorgchem.1c02809
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Stoichiometrically Controlled Assembly of Lanthanide Molecular Complexes of the Heteroditopic Divergent Ligand 4′-(4-Pyridyl)-2,2′:6′,2″-terpyridine N-Oxide in Hypodentate or Bridging Coordination Modes. Structural, Magnetic, and Photoluminescence Studies

Abstract: Mononuclear rare-earth tris-β-diketonato complexes RE­(tta)3dme [RE = Y (1), La (2), Dy (3), or Eu (4); Htta = 2-thenoylacetone; dme = 1,2-dimethoxyethane] react cleanly at room temperature in a 1:1 molar ratio with the heteroditopic divergent ligand 4′-(4-pyridyl)-2,2′:6′,2″-terpyridine N-oxide (pyterpyNO) to yield RE2(tta)6(pyterpyNO) n , where n = 2 for RE = Y (5), Dy (6), or Eu (7) and n = 3 for RE = La (8). The crystal structure of 5 revealed a dinuclear compound with two pyterpyNO’s bridging through the … Show more

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Cited by 13 publications
(33 citation statements)
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“…The dynamics of the magnetization of compound 5 are reported in Figure S9 as temperature dependence of the inphase and out-of-phase magnetic susceptibilities measured without static field applied for eleven sweeping frequencies of the oscillating field. As previously observed for the homometallic Dy 4 (tta) 12 (pyterpyNO) 2 analogue of 5, [70] two sets of peaks appear in the out-of-phase susceptibility, which move to higher temperature upon increase in sweeping frequency, highlighting a Single Molecule Magnet behaviour. A fitting procedure of these peaks using an extended Debye model has been carried out (Figure S9); however, due to the high uncertainty in the determination of the magnetic relaxation times of the faster process, only the relaxation times of the slower one have been taken in consideration in the following discussion, and their temperature dependence is reported in Figure S10.…”
Section: Magnetic Study Ofsupporting
confidence: 74%
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“…The dynamics of the magnetization of compound 5 are reported in Figure S9 as temperature dependence of the inphase and out-of-phase magnetic susceptibilities measured without static field applied for eleven sweeping frequencies of the oscillating field. As previously observed for the homometallic Dy 4 (tta) 12 (pyterpyNO) 2 analogue of 5, [70] two sets of peaks appear in the out-of-phase susceptibility, which move to higher temperature upon increase in sweeping frequency, highlighting a Single Molecule Magnet behaviour. A fitting procedure of these peaks using an extended Debye model has been carried out (Figure S9); however, due to the high uncertainty in the determination of the magnetic relaxation times of the faster process, only the relaxation times of the slower one have been taken in consideration in the following discussion, and their temperature dependence is reported in Figure S10.…”
Section: Magnetic Study Ofsupporting
confidence: 74%
“…First, we assume that, for both molecules, the slow relaxing magnetic moment arises from the dinuclear Dy 2 core, featuring Dy 3 + ions with an antiferromagnetic exchange channelled through the two bridging oxygen atoms, and not from the nona-coordinated Dy 3 + ions located in position 2. Such an assumption is supported by the slight decrease in the magnetic relaxation time upon passing from zero to 1 kOe static field applied (Figure S11), a phenomenon typical of coupled dysprosium(III) Single Molecule Magnets and, as such, observed also for Dy 4 , [70] while it is unusual for uncoupled Dy 3 + Single Ion Magnets. Moreover, this treatment relies on the assumption that the dipolar field acting on the slow relaxing Dy 2 core is the same for 5 and Dy 4 .…”
Section: Magnetic Study Ofmentioning
confidence: 77%
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