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Электронный каталог: Shvanskaya, L. V. - Peculiar Crystal Structure and Strong-Rung Spin Ladders in KCu&sub(2)BiO&sub(2)(SO&sub(4))&sub(2)
Shvanskaya, L. V. - Peculiar Crystal Structure and Strong-Rung Spin Ladders in KCu&sub(2)BiO&sub(2)(SO&sub(4))&sub(2)
Статья
Автор: Shvanskaya, L. V.
Inorganic Chemistry: Peculiar Crystal Structure and Strong-Rung Spin Ladders in KCu&sub(2)BiO&sub(2)(SO&sub(4))&sub(2)
б.г.
ISBN отсутствует
Автор: Shvanskaya, L. V.
Inorganic Chemistry: Peculiar Crystal Structure and Strong-Rung Spin Ladders in KCu&sub(2)BiO&sub(2)(SO&sub(4))&sub(2)
б.г.
ISBN отсутствует
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Статья
Shvanskaya, L.V.
Peculiar Crystal Structure and Strong-Rung Spin Ladders in KCu&sub(2)BiO&sub(2)(SO&sub(4))&sub(2) / L.V.Shvanskaya, P.A.Maksimov, [a.o.]. – Text : electronic // Inorganic Chemistry. – 2026. – Vol. 65, No. 1. – P. 395–402. – URL: https://doi.org/10.1021/acs.inorgchem.5c04485.
KCu&sub(2)BiO&sub(2)(SO&sub(4))&sub(2) has been grown by chemical vapor transport and characterized by single-crystal X-ray diffraction. It crystallizes in the orthorhombic Pnma space group with a = 22.8761(8), b = 5.1961(2), c = 7.2083(2) Å, V = 856.83(5) Å3, Z = 4. Its peculiar crystal structure is organized by heteropolyhedral layers built by edge- and vertex-sharing CuO&sub(5) and BiO&sub(8) polyhedra. Potassium cations are embedded between the layers, which are additionally reinforced by the SO&sub(4) tetrahedra. The temperature dependence of magnetic susceptibility evidences a broad hump at T&sub(max) ∼122 K, accompanied by the Curie tail at lowest temperatures, while the temperature dependence of specific heat features no anomalies ascribable to the phase transition in the whole temperature range. Ab initio calculations demonstrate that the exchange interaction pattern in this material is highly nontrivial. A specific orbital ordering results in the strongest coupling being that of the third-nearest neighbors. This leads to the formation of a spin ladder, a structure that is not directly apparent from crystallographic considerations. There are strong antiferromagnetic interactions on both the rung (J′ = 264 K) and leg (J = 140 K) of the ladder, which result in an energy gap of *D = 161 K in the magnetic excitation spectrum. The Pade approximation of the experimental data provides somewhat lower values of J′ = 205 and J = 117 K, yielding an energy gap of *D = 121 K. The ground state of KCu&sub(2)BiO&sub(2)(SO&sub(4))&sub(2) is a robust quantum spin liquid.
Спец.(статьи,препринты) = С 326.3 - Ферми-системы. Спиновые системы
Спец.(статьи,препринты) = С 36 - Физика твердого тела$
Спец.(статьи,препринты) = С 332.8 - Синхротронное излучение. Лазеры на свободных электронах. Получение и использование рентгеновских лучей
Спец.(статьи,препринты) = С 45 - Физическая химия
ОИЯИ = ОИЯИ (JINR)2026
Shvanskaya, L.V.
Peculiar Crystal Structure and Strong-Rung Spin Ladders in KCu&sub(2)BiO&sub(2)(SO&sub(4))&sub(2) / L.V.Shvanskaya, P.A.Maksimov, [a.o.]. – Text : electronic // Inorganic Chemistry. – 2026. – Vol. 65, No. 1. – P. 395–402. – URL: https://doi.org/10.1021/acs.inorgchem.5c04485.
KCu&sub(2)BiO&sub(2)(SO&sub(4))&sub(2) has been grown by chemical vapor transport and characterized by single-crystal X-ray diffraction. It crystallizes in the orthorhombic Pnma space group with a = 22.8761(8), b = 5.1961(2), c = 7.2083(2) Å, V = 856.83(5) Å3, Z = 4. Its peculiar crystal structure is organized by heteropolyhedral layers built by edge- and vertex-sharing CuO&sub(5) and BiO&sub(8) polyhedra. Potassium cations are embedded between the layers, which are additionally reinforced by the SO&sub(4) tetrahedra. The temperature dependence of magnetic susceptibility evidences a broad hump at T&sub(max) ∼122 K, accompanied by the Curie tail at lowest temperatures, while the temperature dependence of specific heat features no anomalies ascribable to the phase transition in the whole temperature range. Ab initio calculations demonstrate that the exchange interaction pattern in this material is highly nontrivial. A specific orbital ordering results in the strongest coupling being that of the third-nearest neighbors. This leads to the formation of a spin ladder, a structure that is not directly apparent from crystallographic considerations. There are strong antiferromagnetic interactions on both the rung (J′ = 264 K) and leg (J = 140 K) of the ladder, which result in an energy gap of *D = 161 K in the magnetic excitation spectrum. The Pade approximation of the experimental data provides somewhat lower values of J′ = 205 and J = 117 K, yielding an energy gap of *D = 121 K. The ground state of KCu&sub(2)BiO&sub(2)(SO&sub(4))&sub(2) is a robust quantum spin liquid.
Спец.(статьи,препринты) = С 326.3 - Ферми-системы. Спиновые системы
Спец.(статьи,препринты) = С 36 - Физика твердого тела$
Спец.(статьи,препринты) = С 332.8 - Синхротронное излучение. Лазеры на свободных электронах. Получение и использование рентгеновских лучей
Спец.(статьи,препринты) = С 45 - Физическая химия
ОИЯИ = ОИЯИ (JINR)2026
