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Interplay of Anisotropic Exchange Interactions and Single-Ion Anisotropy in Single-Chain Magnets Built from Ru/Os Cyanidometallates(III) and Mn(III) Complex.
- Source :
- Molecules; Feb2023, Vol. 28 Issue 3, p1516, 21p
- Publication Year :
- 2023
-
Abstract
- Two novel 1D heterobimetallic compounds {[Mn<superscript>III</superscript>(SB<superscript>2+</superscript>)M<superscript>III</superscript>(CN)<subscript>6</subscript>]·4H<subscript>2</subscript>O}<subscript>n</subscript> (SB<superscript>2+</superscript> = N,N′-ethylenebis(5-trimethylammoniomethylsalicylideneiminate) based on orbitally degenerate cyanidometallates [Os<superscript>III</superscript>(CN)<subscript>6</subscript>]<superscript>3−</superscript> (1) and [Ru<superscript>III</superscript>(CN)<subscript>6</subscript>]<superscript>3−</superscript> (2) and Mn<superscript>III</superscript> Schiff base complex were synthesized and characterized structurally and magnetically. Their crystal structures consist of electrically neutral, well-isolated chains composed of alternating [M<superscript>III</superscript>(CN)<subscript>6</subscript>]<superscript>3−</superscript> anions and square planar [Mn<superscript>III</superscript>(SB<superscript>2+</superscript>)]<superscript>3+</superscript> cations bridged by cyanide groups. These -ion magnetic anisotropy of Mn<superscript>III</superscript> centers. These results indicate that the presence of compounds exhibit single-chain magnet (SCM) behavior with the energy barriers of Δτ<subscript>1</subscript>/k<subscript>B</subscript> = 73 K, Δτ<subscript>2</subscript>/k<subscript>B</subscript> = 41.5 K (1) and Δτ<subscript>1</subscript>/k<subscript>B</subscript> = 51 K, Δτ<subscript>2</subscript> = 27 K (2). Blocking temperatures of T<subscript>B</subscript> = 2.8, 2.1 K and magnetic hysteresis with coercive fields (at 1.8 K) of 8000, 1600 Oe were found for 1 and 2, respectively. Theoretical analysis of the magnetic data reveals that their single-chain magnet behavior is a product of a complicated interplay of extremely anisotropic triaxial exchange interactions in M<superscript>III</superscript>(4d/5d)–CN–Mn<superscript>III</superscript> fragments: −J<subscript>x</subscript>S<subscript>M</subscript><superscript>x</superscript>S<subscript>Mn</subscript><superscript>x</superscript>−J<subscript>y</subscript>S<subscript>M</subscript><superscript>y</superscript>S<subscript>Mn</subscript><superscript>y</superscript>−J<subscript>z</subscript>S<subscript>M</subscript><superscript>z</superscript>S<subscript>Mn</subscript><superscript>z</superscript>, with opposite sign of exchange parameters J<subscript>x</subscript> = −22, J<subscript>y</subscript> = +28, J<subscript>z</subscript> = −26 cm<superscript>−1</superscript> and J<subscript>x</subscript> = −18, J<subscript>y</subscript> = +20, J<subscript>z</subscript> = −18 cm<superscript>−1</superscript> in 1 and 2, respectively) and single orbitally degenerate [Os<superscript>III</superscript>(CN)<subscript>6</subscript>]<superscript>3−</superscript> and [Ru<superscript>III</superscript>(CN)<subscript>6</subscript>]<superscript>3−</superscript> spin units with unquenched orbital angular momentum in the chain compounds 1 and 2 leads to a peculiar regime of slow magnetic relaxation, which is beyond the scope of the conventional Glaubers's 1D Ising model and anisotropic Heisenberg model. [ABSTRACT FROM AUTHOR]
Details
- Language :
- English
- ISSN :
- 14203049
- Volume :
- 28
- Issue :
- 3
- Database :
- Complementary Index
- Journal :
- Molecules
- Publication Type :
- Academic Journal
- Accession number :
- 161858180
- Full Text :
- https://doi.org/10.3390/molecules28031516