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Title: The structure and weak ferromagnetism of the double layered cuprocobaltate: Y[sub 2]SrCu[sub 0. 6]Co[sub 1. 4]O[sub 6. 5]

Journal Article · · Journal of Solid State Chemistry
 [1]; ;  [2]
  1. Max-Planck-Inst. fuer Festkoerperforschung, Stuttgart (Germany) Univ. of Science and Technology of China, Hefei, Anhui (China)
  2. Max-Planck-Inst. fuer Festkoerperforschung, Stuttgart (Germany)

Rietveld refinement of the X-ray powder diffraction (XRPD) pattern confirms that Y[sub 2]SrCu[sub 0.6]Co[sub 1.4]O[sub 6.5] is isostructural to Y[sub 2]SrCuFeO[sub 6.5]. Unlike its Fe-analog which is antiferromagnetic, Y[sub 2]SrCu[sub 0.6]Co[sub 1.4]O[sub 6.5] behaves as a three-dimensional (3D) ferromagnetic below [Tc] = 385 K with a spontaneous magnetic moment per formula unit of only [mu][sub s] = 0.07[mu][sub B] extrapolated to T = 0 K. The authors concluded that this weak ferromagnetism (WFM) originates from Dzyaloshinsky-Moriya (D-M) spin canting mechanism based on the observation of T[sup 2] dependence of the low-temperature magnetization. The electrical resistance of sintered samples shows an exponential dependence on temperature expo(T[sub 0]/T)[sup [alpha]] with [alpha] = 1/2 in the 185--570 K temperature range, which indicates the conduction mechanism is within variable range hopping (VRH) regime with long-range Coulomb interaction between the carriers. Y[sub 2]SrCu[sub 0.6]Co[sub 1.4]O[sub 6.5] does not show any significant magneto-resistance effect in the 200--400 K temperature range.

OSTI ID:
6068122
Journal Information:
Journal of Solid State Chemistry, Vol. 146:2; ISSN 0022-4596
Country of Publication:
United States
Language:
English

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