Controlled Frustration Release on the Kagome Lattice by Uniaxial-Strain Tuning

Wang, Jierong; Spitaler, M.; Su, Y.-S.; Zoch, K. M.; Krellner, C.; Puphal, P.; Brown, S. E.; Pustogow, A.

doi:10.1103/physrevlett.131.256501

Phys. Rev. Lett.

2023

DOI: 10.1103/physrevlett.131.256501

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Controlled Frustration Release on the Kagome Lattice by Uniaxial-Strain Tuning

Jierong Wang,

M. Spitaler,

Y.-S. Su

et al.

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2024

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Cited by 3 publications

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NMR evidence of spinon localization in the kagome antiferromagnet YCu3(OH)6Br2[Br1−x
Li,
Cui,
Zeng
et al. 2024
Phys. Rev. B
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Magnetic ground states in the kagome system YCu3(OH)6[(ClxBr1−x
Xu,
Shen,
Liu
et al. 2024
Phys. Rev. B
0
0
0
0
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SrCu(OH)3Cl , an isolated equilateral triangle spin S=1/2 model system

Pal,

Doležal,

Strøm

et al. 2024

Phys. Rev. Research

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We have investigated the magnetic ground state properties of the quantum spin trimer compound strontium hydroxy copper chloride SrCu(OH)3Cl using bulk magnetization, specific heat measurements, nuclear magnetic resonance (NMR), and electron spin resonance (ESR) spectroscopy. SrCu(OH)3Cl consists of layers with isolated Cu2+ triangles and hence provides an opportunity to understand the magnetic ground state of an isolated system of S = 1/2 arranged on an equilateral triangle. Although magnetization measurements do not exhibit a phase transition to a long-range ordered state down to T = 2 K, they reveal the characteristic behavior of isolated trimers with an exchange of J=154 K. The Curie-Weiss behavior changes around 50–80 K, as is also seen in the NMR spin-lattice relaxation rate. In zero magnetic field, our specific heat data establish a second-order phase transition to an antiferromagnetic ground state below T= 1.2 K. We have drawn a magnetic field-temperature (H−T) phase diagram based on the specific heat measurements. The ESR data show divergence of the linewidth at lower temperatures, which precedes the phase transition to an antiferromagnetic long-range ordered state with unconventional critical exponents. The temperature variation of the g-factor further confirms the antiferromagnetic phase transition and reflects the underlying magnetocrystalline anisotropy of the compound. Published by the American Physical Society 2024

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Controlled Frustration Release on the Kagome Lattice by Uniaxial-Strain Tuning

Cited by 3 publications

References 56 publications

NMR evidence of spinon localization in the kagome antiferromagnet YCu3(OH)6Br2[Br1−x
Li,
Cui,
Zeng
et al. 2024
Phys. Rev. B
1
0
0
0
View full text Add to dashboard Cite

NMR evidence of spinon localization in the kagome antiferromagnet YCu3(OH)6Br2[Br1−x
Li,
Cui,
Zeng
et al. 2024
Phys. Rev. B
1
0
0
0
View full text Add to dashboard Cite

Magnetic ground states in the kagome system YCu3(OH)6[(ClxBr1−x
Xu,
Shen,
Liu
et al. 2024
Phys. Rev. B
0
0
0
0
View full text Add to dashboard Cite

SrCu(OH)3Cl , an isolated equilateral triangle spin S=1/2 model system

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Controlled Frustration Release on the Kagome Lattice by Uniaxial-Strain Tuning

Cited by 3 publications

References 56 publications

NMR evidence of spinon localization in the kagome antiferromagnet YCu3(OH)6Br2[Br1−xLi, Cui, Zeng et al. 2024Phys. Rev. B1000View full textAdd to dashboardCite

NMR evidence of spinon localization in the kagome antiferromagnet YCu3(OH)6Br2[Br1−xLi, Cui, Zeng et al. 2024Phys. Rev. B1000View full textAdd to dashboardCite

Magnetic ground states in the kagome system YCu3(OH)6[(ClxBr1−xXu, Shen, Liu et al. 2024Phys. Rev. B0000View full textAdd to dashboardCite

SrCu(OH)3Cl , an isolated equilateral triangle spin S=1/2 model system

Contact Info

Product

Resources

About

NMR evidence of spinon localization in the kagome antiferromagnet YCu3(OH)6Br2[Br1−x
Li,
Cui,
Zeng
et al. 2024
Phys. Rev. B
1
0
0
0
View full text Add to dashboard Cite

NMR evidence of spinon localization in the kagome antiferromagnet YCu3(OH)6Br2[Br1−x
Li,
Cui,
Zeng
et al. 2024
Phys. Rev. B
1
0
0
0
View full text Add to dashboard Cite

Magnetic ground states in the kagome system YCu3(OH)6[(ClxBr1−x
Xu,
Shen,
Liu
et al. 2024
Phys. Rev. B
0
0
0
0
View full text Add to dashboard Cite