Non-collinear long-range magnetic ordering in HgCr2S4

(2006)

Authors:

LC Chapon, PG Radaelli, YS Hor, MTF Telling, JF Mitchell

Non-collinear long-range magnetic ordering in HgCr2S4

ArXiv cond-mat/0608031 (2006)

Authors:

LC Chapon, PG Radaelli, YS Hor, MTF Telling, JF Mitchell

Abstract:

The low-temperature magnetic structure of \HG has been studied by high-resolution powder neutron diffraction. Long-range incommensurate magnetic order sets in at T$_N\sim$22K with propagation vector \textbf{k}=(0,0,$\sim$0.18). On cooling below T$_N$, the propagation vector increases and saturates at the commensurate value \textbf{k}=(0,0,0.25). The magnetic structure below T$_N$ consists of ferromagnetic layers in the \textit{ab}-plane stacked in a spiral arrangement along the \textit{c}-axis. Symmetry analysis using corepresentations theory reveals a point group symmetry in the ordered magnetic phase of 422 (D$_4$), which is incompatible with macroscopic ferroelectricity. This finding indicates that the spontaneous electric polarization observed experimentally cannot be coupled to the magnetic order parameter.

Structural and Magnetic Properties of the Kagome Antiferromagnet YbBaCo4O7.

ChemInform Wiley 37:27 (2006) no-no

Authors:

A Huq, JF Mitchell, H Zheng, LC Chapon, PG Radaelli, KS Knight, PW Stephens

Competing magnetic interactions in the extended Kagome system YBaCo4O7

(2006)

Authors:

LC Chapon, PG Radaelli, H Zheng, JF Mitchell

Competing magnetic interactions in the extended Kagome system YBaCo4O7

ArXiv cond-mat/0605307 (2006)

Authors:

LC Chapon, PG Radaelli, H Zheng, JF Mitchell

Abstract:

YBaCo4O7 belongs to a new class of geometrically frustrated magnets like the pyrochlores, in which Co-spins occupy corners of tetrahedra. The structure can be viewed as an alternating stacking of Kagome and triangular layers. Exactly half of the triangular units of the Kagome plane are capped by Co ions to form columns running perpendicular to the Kagome sheets. Neutron powder diffraction reveals a broad temperature range of diffuse magnetic scattering, followed by long range magnetic ordering below 110K. A unique low-temperature magnetic structure simultaneously satisfies an S=0 arrangement in the uncapped triangular units and antiferromagnetic coupling along the columns. A spin reorientation above 30K tracks the relative strengths of the in-plane and out-of-plane interactions.