International audienceMagnetisation measurements and electron spin resonance (ESR) spectra of a doped quasi two dimensional (2D) antiferromagnet on a triangular lattice Rb1-xKxFe(MoO4)(2) reveal a crucial change of the ground state spin configuration and a disappearance of a characteristic 1/3-magnetisation plateau at x = 0.15. According to theory for triangular antiferromagnets with a weak random modulation of the exchange bonds, this is a result of the competition between the structural and dynamic disorders. The dynamic zero-point or thermal fluctuations are known to lift the degeneracy of the mean field ground state of a triangular antiferromagnet and cause the spin configuration to be the most collinear, while the static disorder provi...
The magnetic H amp; 8722;T phase diagram of a quasi two dimensional antiferromagnet RbFe MoO4 2 S 5...
The temperature versus magnetic field phase diagram of the 2D triangular lattice and multiferroic co...
We report the first direct transition from a paramagnetic and paraelectric phase to an incommensurat...
International audienceMagnetisation measurements and electron spin resonance (ESR) spectra of a dope...
International audienceWe observe a disappearance of the 1/3 magnetization plateau and a striking cha...
We observe a disappearance of the 1/3 magnetization plateau and a striking change of the magnetic co...
RbFe(MoO4)(2) is a rare example of a nearly two-dimensional Heisenberg antiferromagnet on a triangul...
RbFe(MoO4)(2) is a rare example of a nearly two-dimensional Heisenberg antiferromagnet on a triangul...
We report temperature-dependent x-ray powder diffraction patterns and single-crystal electron spin r...
We report temperature-dependent x-ray powder diffraction patterns and single-crystal electron spin r...
The static and resonance properties of a quasi-two-dimensional antiferromagnet phase on a distorted ...
We have studied the magnetic and thermodynamic properties as well as the NMR spectra of the quasi-tw...
We report the first direct transition from a paramagnetic and paraelectric phase to an incommensurat...
RbFe(MoO4)(2) is a quasi-two-dimensional (quasi-2D) triangular lattice antiferromagnet (TLA) that di...
The magnetic H − T phase diagram of a quasi-two-dimensional antiferromagnet RbFe(MoO4 )2 (S = 5/2) w...
The magnetic H amp; 8722;T phase diagram of a quasi two dimensional antiferromagnet RbFe MoO4 2 S 5...
The temperature versus magnetic field phase diagram of the 2D triangular lattice and multiferroic co...
We report the first direct transition from a paramagnetic and paraelectric phase to an incommensurat...
International audienceMagnetisation measurements and electron spin resonance (ESR) spectra of a dope...
International audienceWe observe a disappearance of the 1/3 magnetization plateau and a striking cha...
We observe a disappearance of the 1/3 magnetization plateau and a striking change of the magnetic co...
RbFe(MoO4)(2) is a rare example of a nearly two-dimensional Heisenberg antiferromagnet on a triangul...
RbFe(MoO4)(2) is a rare example of a nearly two-dimensional Heisenberg antiferromagnet on a triangul...
We report temperature-dependent x-ray powder diffraction patterns and single-crystal electron spin r...
We report temperature-dependent x-ray powder diffraction patterns and single-crystal electron spin r...
The static and resonance properties of a quasi-two-dimensional antiferromagnet phase on a distorted ...
We have studied the magnetic and thermodynamic properties as well as the NMR spectra of the quasi-tw...
We report the first direct transition from a paramagnetic and paraelectric phase to an incommensurat...
RbFe(MoO4)(2) is a quasi-two-dimensional (quasi-2D) triangular lattice antiferromagnet (TLA) that di...
The magnetic H − T phase diagram of a quasi-two-dimensional antiferromagnet RbFe(MoO4 )2 (S = 5/2) w...
The magnetic H amp; 8722;T phase diagram of a quasi two dimensional antiferromagnet RbFe MoO4 2 S 5...
The temperature versus magnetic field phase diagram of the 2D triangular lattice and multiferroic co...
We report the first direct transition from a paramagnetic and paraelectric phase to an incommensurat...