Structures of magnetic excitations in the spin-1/2 kagome-lattice antiferromagnets Cs$_2$Cu$_3$SnF$_{12}$ and Rb$_2$Cu$_3$SnF$_{12}$

Mutsuki Saito; Ryunosuke Takagishi; Nobuyuki Kurita; Masari Watanabe; Hidekazu Tanaka; Ryuji Nomura; Yoshiyuki Fukumoto; Kazuhiko Ikeuchi; Ryoichi Kajimoto

doi:10.1103/PhysRevB.105.064424

paper

Structures of magnetic excitations in the spin-1/2 kagome-lattice antiferromagnets Cs $_{2}$ Cu $_{3}$ SnF $_{12}$ and Rb $_{2}$ Cu $_{3}$ SnF $_{12}$

arXiv:2112.00934 · doi:10.1103/PhysRevB.105.064424

Abstract

We show the structures of magnetic excitations in spin-1/2 kagome-lattice antiferromagnets Cs $_{2}$ Cu $_{3}$ SnF $_{12}$ and Rb $_{2}$ Cu $_{3}$ SnF $_{12}$ investigated by inelastic neutron scattering in wide energy and momentum ranges. For Cs $_{2}$ Cu $_{3}$ SnF $_{12}$ , four single-magnon excitation modes were observed. Low-energy three modes are assigned to be transverse modes and the high-energy fourth mode is suggested to be an amplitude mode. It was found that the broad excitation continuum without a marked structure spreads in a wide energy range from $0.15 J$ to approximately $2.5 J$ in contrast to the clearly structured excitation continuum observed in the spin-1/2 triangular-lattice Heisenberg antiferromagnet. These findings strongly suggest spinon excitations as elementary excitations in Cs $_{2}$ Cu $_{3}$ SnF $_{12}$ . In Rb $_{2}$ Cu $_{3}$ SnF $_{12}$ , singlet-triplet excitations from the pinwheel VBS state and their ghost modes caused by the enlargement of the chemical unit cell were clearly confirmed. It was found that the excitation continuum is structured in the low-energy region approximately below $J_{avg}$ and the almost structureless high-energy excitation continuum extends to approximately $2.6 J_{avg}$ . The characteristics of the high-energy excitation continuum are common to both Cs $_{2}$ Cu $_{3}$ SnF $_{12}$ and Rb $_{2}$ Cu $_{3}$ SnF $_{12}$ , irrespective of their ground states. The experimental results strongly suggest that the spin liquid component remains in the ground state as quantum fluctuations in Cs $_{2}$ Cu $_{3}$ SnF $_{12}$ and Rb $_{2}$ Cu $_{3}$ SnF $_{12}$ .

arXiv comment15 pages, 7 figures

Structures of magnetic excitations in the spin-1/2 kagome-lattice antiferromagnets Cs $_{2}$ Cu $_{3}$ SnF $_{12}$ and Rb $_{2}$ Cu $_{3}$ SnF $_{12}$

Abstract

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Structures of magnetic excitations in the spin-1/2 kagome-lattice antiferromagnets Cs2​Cu3​SnF12​ and Rb2​Cu3​SnF12​

Abstract

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Structures of magnetic excitations in the spin-1/2 kagome-lattice antiferromagnets Cs $_{2}$ Cu $_{3}$ SnF $_{12}$ and Rb $_{2}$ Cu $_{3}$ SnF $_{12}$