Frustrated magnets with a strong spin-lattice coupling can show rich magnetic phases and the associated fascinating phenomena. A promising platform is the breathing pyrochlore magnet CuInCr$_{4}$S$_{8}$ with localized $S=3/2$ Cr$^{3+}$ ions, which is proposed to be effectively viewed as an $S=6$ Heisenberg antiferromagnet on the face-centered-cubic lattice. Here, we unveil that CuInCr$_{4}$S$_{8}$ exhibits a complex magnetic phase diagram with a small phase pocket ($A$ phase) by means of magnetization, magnetostriction, magnetocapacitance, and magnetocaloric-effect measurements in pulsed high magnetic fields of up to 60 T. Remarkably, the appearance of $A$ phase is accompanied by anomalous magnetostrictive and magnetocapacitive responses, s...
We report on a heat-capacity study of high-quality single-crystal samples of LiCuVO4 — a frustrated ...
We investigate the structural and magnetic properties of two molecule-based magnets synthesized from...
The V-based kagome systems AV3Sb5 (A = Cs, Rb and K) are unique by virtue of the intricate interplay...
In frustrated magnetic systems, the competition amongst interactions can introduce extremely high de...
Cs2CuCl4 is known to possess a quantum spin-liquid phase with antiferromagnetic interaction below 2....
We present the synthesis and physical properties of a new breathing pyrochlore magnet CuAlCr$_4$S$_8...
We present a theoretical analysis of the magnetocaloric effect in the frustrated antiferromagnet \Eu...
We study the $S=1/2$ pyrochlore Heisenberg antiferromagnet in a magnetic field. Using large scale de...
Magnetic frustration, the competition among exchange interactions, often leads to novel magnetic gro...
Two triangular lattice antiferromagnets Sr$_3$Co(Nb,Ta)$_2$O$_9$ with an effective $j_{\rm eff}=1/2$...
It is predicted that strongly interacting spins on a frustrated lattice may lead to a quantum disord...
Proximity to magnetic order as well as low dimensionality are both beneficial to superconductivity a...
We investigate the effects of diamagnetic doping in the solid-solution series $Tb_{1-x}Y_{x}(HCO_{2}...
Geometrically frustrated structures combined with competing exchange interactions that have differen...
Magnetic frustration, the competition among exchange interactions, often leads to novel magnetic gro...
We report on a heat-capacity study of high-quality single-crystal samples of LiCuVO4 — a frustrated ...
We investigate the structural and magnetic properties of two molecule-based magnets synthesized from...
The V-based kagome systems AV3Sb5 (A = Cs, Rb and K) are unique by virtue of the intricate interplay...
In frustrated magnetic systems, the competition amongst interactions can introduce extremely high de...
Cs2CuCl4 is known to possess a quantum spin-liquid phase with antiferromagnetic interaction below 2....
We present the synthesis and physical properties of a new breathing pyrochlore magnet CuAlCr$_4$S$_8...
We present a theoretical analysis of the magnetocaloric effect in the frustrated antiferromagnet \Eu...
We study the $S=1/2$ pyrochlore Heisenberg antiferromagnet in a magnetic field. Using large scale de...
Magnetic frustration, the competition among exchange interactions, often leads to novel magnetic gro...
Two triangular lattice antiferromagnets Sr$_3$Co(Nb,Ta)$_2$O$_9$ with an effective $j_{\rm eff}=1/2$...
It is predicted that strongly interacting spins on a frustrated lattice may lead to a quantum disord...
Proximity to magnetic order as well as low dimensionality are both beneficial to superconductivity a...
We investigate the effects of diamagnetic doping in the solid-solution series $Tb_{1-x}Y_{x}(HCO_{2}...
Geometrically frustrated structures combined with competing exchange interactions that have differen...
Magnetic frustration, the competition among exchange interactions, often leads to novel magnetic gro...
We report on a heat-capacity study of high-quality single-crystal samples of LiCuVO4 — a frustrated ...
We investigate the structural and magnetic properties of two molecule-based magnets synthesized from...
The V-based kagome systems AV3Sb5 (A = Cs, Rb and K) are unique by virtue of the intricate interplay...