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Engineering of the XY Magnetic Layered System with Adeninium Cations: Monocrystalline Angle-Resolved Studies of Nonlinear Magnetic Susceptibility

[Image: see text] An original example of modular crystal engineering involving molecular magnetic {Cu(II)[W(V)(CN)(8)]}(−) bilayers and adeninium cations (AdeH(+)) toward the new layered molecular magnet (AdeH){Cu(II)[W(V)(CN)(8)]}·2H(2)O (1) is presented. 1 crystallizes within the monoclinic C2 spa...

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Detalles Bibliográficos
Autores principales: Kuzniak-Glanowska, Emilia, Konieczny, Piotr, Pełka, Robert, Muzioł, Tadeusz M., Kozieł, Marcin, Podgajny, Robert
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2021
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8388120/
https://www.ncbi.nlm.nih.gov/pubmed/34232628
http://dx.doi.org/10.1021/acs.inorgchem.1c00432
Descripción
Sumario:[Image: see text] An original example of modular crystal engineering involving molecular magnetic {Cu(II)[W(V)(CN)(8)]}(−) bilayers and adeninium cations (AdeH(+)) toward the new layered molecular magnet (AdeH){Cu(II)[W(V)(CN)(8)]}·2H(2)O (1) is presented. 1 crystallizes within the monoclinic C2 space group (a = 41.3174(12), b = 7.0727(3), c = 7.3180(2) Å, β = 93.119(3)°, and V = 2135 Å(3)). The bilayer topology is based on a stereochemical matching between the square pyramidal shape of Cu(II) moiety and the bicapped trigonal prismatic shape of [W(V)(μ-CN)(5)(CN)(3)], and the separation between bilayers is significantly increased (by ∼50%; from ca. 9.5 to ca. 14.5 Å) compared to several former analogues in this family. This was achieved via a unique combination of (i) a 1D ribbonlike hydrogen bond system {AdeH(+)···H(2)O···AdeH(+)···}(∞) exploiting planar water-assisted Hoogsteen···Sugar synthons with (ii) parallel 1D π–π stacks {AdeH(+)···AdeH(+)}(∞). In-plane 2D XY magnetism is characterized by a T(c) close to 33 K, H(c,in-plane) = 60 Oe, and H(c,out-of-plane) = 750 Oe, high values of in-plane γ critical exponents (γ(b) = 2.34(6) for H||b and γ(c) = 2.16(5) for H||c), and a Berezinskii–Kosterlitz–Thouless (BKT) topological phase transition, deduced from crystal-orientation-dependent scaling analysis. The obtained values of in-plane ν critical exponents, ν(b) = 0.48(5) for H||b and ν(c) = 0.49(3) for H||c, confirm the BKT transition (ν(BKT) = 0.5). Full-range angle-resolved monocrystalline magnetic measurements supported by dedicated calculations indicated the occurrence of nonlinear susceptibility performance within the easy plane in a magnetically ordered state. We refer the occurrence of this phenomenon to spontaneous resolution in the C2 space group, a tandem not observed in studies on previous analogues and rarely reported in the field of molecular materials. The above magneto-supramolecular strategy may provide a novel means for the design of 2D molecular magnetic networks and help to uncover the inherent phenomena.