<p>La<sub>0.7-x</sub>Lu<sub>x</sub>Ca<sub>0.3</sub>MnO<sub>3</sub> manufactured by the ceramic method have been carefully studied. Structural analyses prove the compound with <i>x</i>&#xa0;=&#xa0;0.03 exhibiting the monophase in an orthorhombic structure, similar to the parent compound (<i>x</i>&#xa0;=&#xa0;0). At higher Lu concentrations (<i>x</i>&#xa0;≥&#xa0;0.06), besides the orthorhombic phase, there is an additionally constituted secondary phase of hexagonal LuMnO<sub>3</sub>. This phase together with the replacement of a smaller Lu<sup>3+</sup> ion for a larger La<sup>3+</sup> one in orthorhombic compounds would reduce the magnetization. Comparing to <i>x</i>&#xa0;=&#xa0;0 (<i>T</i><sub><i>C</i></sub> ≈ 252&#xa0;K), the Lu doping at <i>x</i>&#xa0;=&#xa0;0.03 reduced strongly <i>T</i><sub><i>C</i></sub> to&#xa0;~&#xa0;208&#xa0;K. However, as <i>x</i>&#xa0;≥&#xa0;0.06, the <i>T</i><sub><i>C</i></sub> reduction becomes slower, <i>T</i><sub><i>C</i></sub> ≈ 203&#xa0;K for <i>x</i>&#xa0;=&#xa0;0.12. In particular, the Lu doping does not change the phase-transition feature, all compounds still exhibit the first-order character. Near <i>T</i><sub><i>C</i></sub>, the magnetic entropy change is largest of 4.2~5.8&#xa0;J/kg&#xa0;K, while the relative cooling power ranges from 120 to&#xa0;~&#xa0;140&#xa0;J/kg, for a field variation of <i>H</i>&#xa0;=&#xa0;30 kOe. Comparing with LaMnO<sub>3</sub>-based magnetocaloric materials, we believe that La<sub>0.7-x</sub>Lu<sub>x</sub>Ca<sub>0.3</sub>MnO<sub>3</sub> compounds are also potential materials for magnetocaloric applications at temperatures <i>T</i>&#xa0;=&#xa0;200-231&#xa0;K.</p>

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Structural Phase Separation, Magnetic and Magnetocaloric Properties of La0.7-xLuxCa0.3MnO3 Ceramics

  • Kim T. H. My,
  • H. T. Anh,
  • H. N. Nhat,
  • T. D. Thanh,
  • D. H. Manh,
  • T. V. Manh,
  • D. D. Bich,
  • D. T. Khan,
  • N. T. Dang,
  • P. D. Thang,
  • D.-H. Kim,
  • T. L. Phan

摘要

La0.7-xLuxCa0.3MnO3 manufactured by the ceramic method have been carefully studied. Structural analyses prove the compound with x = 0.03 exhibiting the monophase in an orthorhombic structure, similar to the parent compound (x = 0). At higher Lu concentrations (x ≥ 0.06), besides the orthorhombic phase, there is an additionally constituted secondary phase of hexagonal LuMnO3. This phase together with the replacement of a smaller Lu3+ ion for a larger La3+ one in orthorhombic compounds would reduce the magnetization. Comparing to x = 0 (TC ≈ 252 K), the Lu doping at x = 0.03 reduced strongly TC to ~ 208 K. However, as x ≥ 0.06, the TC reduction becomes slower, TC ≈ 203 K for x = 0.12. In particular, the Lu doping does not change the phase-transition feature, all compounds still exhibit the first-order character. Near TC, the magnetic entropy change is largest of 4.2~5.8 J/kg K, while the relative cooling power ranges from 120 to ~ 140 J/kg, for a field variation of H = 30 kOe. Comparing with LaMnO3-based magnetocaloric materials, we believe that La0.7-xLuxCa0.3MnO3 compounds are also potential materials for magnetocaloric applications at temperatures T = 200-231 K.