Planar polycubane single-molecule magnet [Ni^sub 6^(pymeid)^sub 6^Ni^sub 12^(OH)^sub 6^(µ^sub 3^OH)^sub 16^Cl^sub 2^ (H^sub 2^O)^sub 2^]·38H^sub 2^O: Experiment and theory

Comprehensive experimental and theoretical study of atomic and magnetic structure of the 18-nuclei complex [Ni6(pymeid)6Ni12(OH)6(µ3-OH)16Cl2 (H2O)2] 38H2O (H2pymeid – N-(2-pyridyl)methyliminodipropionic acid) with rare polycubane planar architecture is reported. Magnetic moments of NiII ions (S = 1...

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Veröffentlicht in:Inorganica Chimica Acta 2018-11, Vol.483, p.480
Hauptverfasser: Shvachko, YuN, Starichenko, DV, Korolev, AV, Pestov, AV, Slepukhin, PA, Boukhvalov, DW
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container_title Inorganica Chimica Acta
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Starichenko, DV
Korolev, AV
Pestov, AV
Slepukhin, PA
Boukhvalov, DW
description Comprehensive experimental and theoretical study of atomic and magnetic structure of the 18-nuclei complex [Ni6(pymeid)6Ni12(OH)6(µ3-OH)16Cl2 (H2O)2] 38H2O (H2pymeid – N-(2-pyridyl)methyliminodipropionic acid) with rare polycubane planar architecture is reported. Magnetic moments of NiII ions (S = 1) in the sectional metal-oxygen Ni18 core are coupled ferro- and antiferromagnetically, so that the complex is a single-molecule magnet (SMM) with the total spin in the ground state S = 10, and the blocking temperature Tb = 14.3 K. The ac – susceptibility, χ’’, obeys the Arrhenius law with the effective barrier Ueff = 18.9 cm−1 (27.2 K). QTM regime is observed at T ≤ 8 K. Magnetic anisotropy is characterized by remanent magnetization M0 = 0.7 µB and coercive field Hc = 340 Oe. Electronic structure and values of the local moments and the exchange constants are calculated in the LDA + U DFT approach. Two complementary 3-nuclei cubane fragments are linked antiferromagnetically to the main 12-nuclei ferromagnetic core. The ligands moderate the exchange couplings in the adjacent cubanes by shifting respective 3d DOS peaks of peripheral Ni ions towards lower energies.
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Magnetic moments of NiII ions (S = 1) in the sectional metal-oxygen Ni18 core are coupled ferro- and antiferromagnetically, so that the complex is a single-molecule magnet (SMM) with the total spin in the ground state S = 10, and the blocking temperature Tb = 14.3 K. The ac – susceptibility, χ’’, obeys the Arrhenius law with the effective barrier Ueff = 18.9 cm−1 (27.2 K). QTM regime is observed at T ≤ 8 K. Magnetic anisotropy is characterized by remanent magnetization M0 = 0.7 µB and coercive field Hc = 340 Oe. Electronic structure and values of the local moments and the exchange constants are calculated in the LDA + U DFT approach. Two complementary 3-nuclei cubane fragments are linked antiferromagnetically to the main 12-nuclei ferromagnetic core. 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Magnetic moments of NiII ions (S = 1) in the sectional metal-oxygen Ni18 core are coupled ferro- and antiferromagnetically, so that the complex is a single-molecule magnet (SMM) with the total spin in the ground state S = 10, and the blocking temperature Tb = 14.3 K. The ac – susceptibility, χ’’, obeys the Arrhenius law with the effective barrier Ueff = 18.9 cm−1 (27.2 K). QTM regime is observed at T ≤ 8 K. Magnetic anisotropy is characterized by remanent magnetization M0 = 0.7 µB and coercive field Hc = 340 Oe. Electronic structure and values of the local moments and the exchange constants are calculated in the LDA + U DFT approach. Two complementary 3-nuclei cubane fragments are linked antiferromagnetically to the main 12-nuclei ferromagnetic core. The ligands moderate the exchange couplings in the adjacent cubanes by shifting respective 3d DOS peaks of peripheral Ni ions towards lower energies.</abstract><cop>Amsterdam</cop><pub>Elsevier Science Ltd</pub></addata></record>
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subjects Anisotropy
Antiferromagnetism
Atomic structure
Coercivity
Coupling (molecular)
Couplings
Crystal structure
Cubane
Electronic structure
Exchanging
Ferromagnetism
Magnetic anisotropy
Magnetic moments
Magnetic permeability
Magnetic structure
Magnetism
Nuclei (nuclear physics)
title Planar polycubane single-molecule magnet [Ni^sub 6^(pymeid)^sub 6^Ni^sub 12^(OH)^sub 6^(µ^sub 3^OH)^sub 16^Cl^sub 2^ (H^sub 2^O)^sub 2^]·38H^sub 2^O: Experiment and theory
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