The S=1/2 three-leg quantum spin nanotube with the ring exchange interaction is investigated using the numerical exact diagonalization of finte-size clusters and finite-size scaling analysis. The previous study suggested that the ring exchange interaction induces the quantum phase transition from the spin gap phase to some new phase. The present work indicates that the new phase is the spin nematic Tomonaga-Luttinger liquid phase
A quantum spin-liquid phase is an intriguing possibility for a system of strongly interacting magnet...
A quantum spin-liquid phase is an intriguing possibility for a system of strongly interacting magnet...
We study the magnetization plateau state of the three-leg spin-1/2 tube in the strong rung coupling ...
AbstractThe S=1/2 three-leg quantum spin tube is investigated using the numerical diagonalization. T...
AbstractThe S=1/2 three-leg quantum spin tube is investigated using the numerical diagonalization. T...
We investigate the spin-1/2 twisted three-leg antiferromagnetic quantum spin tube in the presence of...
The magnetization process of the S = 1 antiferromagnetic chain with thebiquadratic interaction is in...
The spin nematic phase, which is a kind of multipole phases, has attracted a lot of interest in the ...
Quantum spin ice materials, pyrochlore magnets with competing Ising and transverse exchange interact...
Quantum spin ice materials, pyrochlore magnets with competing Ising and transverse exchange interact...
Quantum spin ice materials, pyrochlore magnets with competing Ising and transverse exchange interact...
Quantum spin ice materials, pyrochlore magnets with competing Ising and transverse exchange interact...
Quantum spin ice materials, pyrochlore magnets with competing Ising and transverse exchange interact...
The magnetization process of the $S=1$ antiferromagnetic chain with the single-ion anisotropy $D$ an...
The quantum spin nanotubes are theoretically investigated using the large-scale numerical diagonaliz...
A quantum spin-liquid phase is an intriguing possibility for a system of strongly interacting magnet...
A quantum spin-liquid phase is an intriguing possibility for a system of strongly interacting magnet...
We study the magnetization plateau state of the three-leg spin-1/2 tube in the strong rung coupling ...
AbstractThe S=1/2 three-leg quantum spin tube is investigated using the numerical diagonalization. T...
AbstractThe S=1/2 three-leg quantum spin tube is investigated using the numerical diagonalization. T...
We investigate the spin-1/2 twisted three-leg antiferromagnetic quantum spin tube in the presence of...
The magnetization process of the S = 1 antiferromagnetic chain with thebiquadratic interaction is in...
The spin nematic phase, which is a kind of multipole phases, has attracted a lot of interest in the ...
Quantum spin ice materials, pyrochlore magnets with competing Ising and transverse exchange interact...
Quantum spin ice materials, pyrochlore magnets with competing Ising and transverse exchange interact...
Quantum spin ice materials, pyrochlore magnets with competing Ising and transverse exchange interact...
Quantum spin ice materials, pyrochlore magnets with competing Ising and transverse exchange interact...
Quantum spin ice materials, pyrochlore magnets with competing Ising and transverse exchange interact...
The magnetization process of the $S=1$ antiferromagnetic chain with the single-ion anisotropy $D$ an...
The quantum spin nanotubes are theoretically investigated using the large-scale numerical diagonaliz...
A quantum spin-liquid phase is an intriguing possibility for a system of strongly interacting magnet...
A quantum spin-liquid phase is an intriguing possibility for a system of strongly interacting magnet...
We study the magnetization plateau state of the three-leg spin-1/2 tube in the strong rung coupling ...