The crystalline and magnetic structures of

{Ca}_{2} {Ru}_{1 - x} {Fe}_{x} O_{4}

(

x = 0.02

, 0.05, 0.08, and 0.12) have been studied using neutron and x-ray diffraction. The Fe-doping reduces the Ru-O bond length in both apical and planar directions. The smaller Ru(

Fe) O_{6}

octahedron leads to its reduced distortion. The

P b c a

space group is maintained in all the Fe dopings, so is the octahedral flattening. Warming has a similar effect on the lattice to that of the Fe doping in releasing the distorted octahedra but precipitates an abrupt octahedral elongation near the

N \overset{́}{e} el

temperature. Two competing antiferromagnetic orders,

A

- and

B

-centered phases have been observed. The Fe-doping-relaxed crystal structure prefers the latter to the former. As the doping increases, the

B

-centered phase continuously grows at the cost of the

A

-centered one and eventually replaces it at

x = 0.12

. The absence of the two-dimensional antiferromagnetic critical fluctuations above the magnetic transition temperature and the three-dimensional magnetic correlation below the transition, together with the anomalous lattice response, point to an important role of orbital degree of freedom in driving the magnetic phase competition.

Publications with shared reference:

0 publications found