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Nonlinear piezomagnetoelectric effect in CuFeO2

Physical review. B, 2019-11, Vol.100 (20), p.1

2019

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Magnetic transitions in botallackite-structure Cu2(OH)3Br and Cu2(OH)3I

Physica. B, Condensed matter, 2009-04, Vol.404 (5-7), p.680-682

2009

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Magnetic field tunable dielectric dispersion in successive field-induced magnetic phases of the geometrically frustrated magnet CuFeO2 up to 28 T

Physical review. B, 2018-06, Vol.97 (21)

2018

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Spin-glass state in the mixed system (Co 1− x Fe x ) 2(OH) 3Cl on deformed pyrochlore lattice

Physica. B, Condensed matter, 2009-04, Vol.404 (5), p.674-676

2009

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Spin gap in the weakly interacting quantum spin chain antiferromagnet KCuPO 4 · H 2 O

Physical review. B, 2023-02, Vol.107 (5), Article 054435

2023

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Cluster-Based Haldane State in an Edge-Shared Tetrahedral Spin-Cluster Chain: Fedotovite K 2 Cu 3 O ( SO 4 ) 3

Physical review letters, 2018-02, Vol.120 (7), Article 077201

2018

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Relief of spin frustration through magnetic anisotropy in the quasi-one-dimensional S = 1 2 antiferromagnet Na 2 CuSO 4 Cl 2

Physical review. B, 2022-04, Vol.105 (14), Article 144410

2022

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Cluster-Based Haldane State in an Edge-Shared Tetrahedral Spin-Cluster Chain: Fedotovite K^sub 2^Cu^sub 3^O( SO^sub 4^)^sub 3

Physical review letters, 2018-02, Vol.120 (7), p.077201

2018

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Nonlinear piezomagnetoelectric effect in CuFeO 2

Physical review. B, 2019-11, Vol.100 (20), Article 201105

2019

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Spin dynamics and magnetic ordering in the quasi-one-dimensional S = 1 2 antiferromagnet Na 2 CuSO 4 Cl 2

Physical review. B, 2020-01, Vol.101 (2), Article 024410

2020

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Spin dynamics and magnetic ordering in the quasi-one-dimensional S=12 antiferromagnet Na2CuSO4Cl2

Physical review. B, 2020-01, Vol.101 (2), p.1

2020

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Spin order in the Heisenberg kagome antiferromagnet MgF e 3 ( OH ) 6 C l 2

Physical review. B, 2017-10, Vol.96 (14), Article 144111

2017

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Spin order in the Heisenberg kagome antiferromagnet MgFe3(OH)6Cl2

Physical review. B, 2017-10, Vol.96 (14)

2017

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Magnetic field tunable dielectric dispersion in successive field-induced magnetic phases of the geometrically frustrated magnet CuFeO 2 up to 28 T

Physical review. B, 2018-06, Vol.97 (21), Article 214407

2018

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Magnetic transitions in botallackite-structure Cu 2(OH) 3Br and Cu 2(OH) 3I

Physica. B, Condensed matter, 2009, Vol.404 (5), p.680-682

2009

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Cluster-Based Haldane State in an Edge-Shared Tetrahedral Spin-Cluster Chain: Fedotovite K_{2}Cu_{3}O(SO_{4})_{3}

Physical review letters, 2018-02, Vol.120 (7), p.077201-077201

2018

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Recent developments in the magnetic study of the deformed pyrochlore lattice M2(OH)3X (M = 3d magnetic ions, X = Cl, Br) - exotic magnetic order in Ni2(OH)3Cl and controlled spin-spin interactions in Co2(OH)3Cl1-xBrx and (Co1-xFex)2(OH)3Cl

Journal of physics. Conference series, 2009-01, Vol.145 (1), p.012034

2009

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Recent developments in the magnetic study of the deformed pyrochlore lattice M 2 (OH) 3 X ( M = 3 d magnetic ions, X = Cl, Br) - exotic magnetic order in Ni 2 (OH) 3 Cl and controlled spin-spin interactions in Co 2 (OH) 3 Cl 1- x Br x and (Co 1- x Fe x ) 2 (OH) 3 Cl

Journal of physics. Conference series, 2009-01, Vol.145, p.12034

2009

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Strong magnetic-dielectric-lattice coupling in transition metal hydroxyhalides and ferroelectric response in rhombohedral Co 2 (OD) 3 X ( X = Cl , Br)

Physical review. B, Condensed matter and materials physics, 2013-05, Vol.87 (17), Article 174102

2013

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Strong magnetic-dielectric-lattice coupling in transition metal hydroxyhalides and ferroelectric response in rhombohedral Co sub(2)(OD) sub(3)X (X = Cl, Br)

Physical review. B, Condensed matter and materials physics, 2013-05, Vol.87 (17)

2013

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Antiferromagnetic magnetic transition and spin fluctuations in the deformed pyrochlore compound β -Fe 2 ( OH ) 3 Cl

Physical review. B, Condensed matter and materials physics, 2010-07, Vol.82 (2), Article 024425

2010

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Short-range correlations and persistent spin fluctuations in the undistorted kagome lattice Ising antiferromagnet Co 3 Mg(OH) 6 Cl 2

Physical review. B, Condensed matter and materials physics, 2012-01, Vol.85 (1), Article 012402

2012

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Short-range correlations and persistent spin fluctuations in the undistorted kagome lattice Ising antiferromagnet Co sub(3)Mg(OH) sub(6)Cl sub(2)

Physical review. B, Condensed matter and materials physics, 2012-01, Vol.85 (1), p.012402-012402

2012

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Two-dimensional triangular-lattice Cu(OH)Cl, belloite, as a magnetodielectric system

Physical review materials, 2018-10, Vol.2 (10), Article 104401

2018

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Nonlinear piezomagnetoelectric effect in CuFeO2

Magnetic transitions in botallackite-structure Cu2(OH)3Br and Cu2(OH)3I

Magnetic field tunable dielectric dispersion in successive field-induced magnetic phases of the geometrically frustrated magnet CuFeO2 up to 28 T

Spin-glass state in the mixed system (Co 1− x Fe x ) 2(OH) 3Cl on deformed pyrochlore lattice

Spin gap in the weakly interacting quantum spin chain antiferromagnet KCuPO 4 · H 2 O

Cluster-Based Haldane State in an Edge-Shared Tetrahedral Spin-Cluster Chain: Fedotovite K 2 Cu 3 O ( SO 4 ) 3

Relief of spin frustration through magnetic anisotropy in the quasi-one-dimensional S = 1 2 antiferromagnet Na 2 CuSO 4 Cl 2

Cluster-Based Haldane State in an Edge-Shared Tetrahedral Spin-Cluster Chain: Fedotovite K^sub 2^Cu^sub 3^O( SO^sub 4^)^sub 3

Nonlinear piezomagnetoelectric effect in CuFeO 2

Spin dynamics and magnetic ordering in the quasi-one-dimensional S = 1 2 antiferromagnet Na 2 CuSO 4 Cl 2

Spin dynamics and magnetic ordering in the quasi-one-dimensional S=12 antiferromagnet Na2CuSO4Cl2

Spin order in the Heisenberg kagome antiferromagnet MgF e 3 ( OH ) 6 C l 2

Spin order in the Heisenberg kagome antiferromagnet MgFe3(OH)6Cl2

Magnetic field tunable dielectric dispersion in successive field-induced magnetic phases of the geometrically frustrated magnet CuFeO 2 up to 28 T

Magnetic transitions in botallackite-structure Cu 2(OH) 3Br and Cu 2(OH) 3I

Cluster-Based Haldane State in an Edge-Shared Tetrahedral Spin-Cluster Chain: Fedotovite K_{2}Cu_{3}O(SO_{4})_{3}

Recent developments in the magnetic study of the deformed pyrochlore lattice M2(OH)3X (M = 3d magnetic ions, X = Cl, Br) - exotic magnetic order in Ni2(OH)3Cl and controlled spin-spin interactions in Co2(OH)3Cl1-xBrx and (Co1-xFex)2(OH)3Cl

Recent developments in the magnetic study of the deformed pyrochlore lattice M 2 (OH) 3 X ( M = 3 d magnetic ions, X = Cl, Br) - exotic magnetic order in Ni 2 (OH) 3 Cl and controlled spin-spin interactions in Co 2 (OH) 3 Cl 1- x Br x and (Co 1- x Fe x ) 2 (OH) 3 Cl

Strong magnetic-dielectric-lattice coupling in transition metal hydroxyhalides and ferroelectric response in rhombohedral Co 2 (OD) 3 X ( X = Cl , Br)

Strong magnetic-dielectric-lattice coupling in transition metal hydroxyhalides and ferroelectric response in rhombohedral Co sub(2)(OD) sub(3)X (X = Cl, Br)

Antiferromagnetic magnetic transition and spin fluctuations in the deformed pyrochlore compound β -Fe 2 ( OH ) 3 Cl

Short-range correlations and persistent spin fluctuations in the undistorted kagome lattice Ising antiferromagnet Co 3 Mg(OH) 6 Cl 2

Short-range correlations and persistent spin fluctuations in the undistorted kagome lattice Ising antiferromagnet Co sub(3)Mg(OH) sub(6)Cl sub(2)

Two-dimensional triangular-lattice Cu(OH)Cl, belloite, as a magnetodielectric system

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