4.8 Article

Structure, magnetism, and magnetoresistance of the compounds Eu14MnAs11 and Eu14MnP11

Journal

CHEMISTRY OF MATERIALS
Volume 13, Issue 4, Pages 1398-1406

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/cm0007050

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The new compounds Eu14MnAs11 and Eu14MnP11 were synthesized from stoichiometric amounts of the elements. The compounds are isotypic to Ca14AlSb11 and crystallize in the tetragonal space group I4(1)/acd (Z = 8). Lattice parameters obtained from single-crystal X-ray diffraction at 130 Ii are alpha = 16.318 (2) Angstrom, c = 21.684 (4) Angstrom and alpha = 15.930 (4) Angstrom, c = 21.213 (5) Angstrom for Eu14MnAs11 and Eu14MnP11, respectively. In the refinement of each structure, the central Pn(4) site of a Pn(3)(7-) linear unit (Pn = As, P) shows positional disorder; this is in contrast to the ordered structures formed when Pn = Sta and Bi, Eu14MnAs11 and Eu14- MnP11 are ferromagnetic with transitions at 74 and 52 K, respectively. Eu14MnAs11 also has a low-temperature transition at similar to 25 K. Resistivity measurements indicate an insulator-to-metal transition near the magnetic transition, and plots of ln rho vs 1/T are linear above To, providing activation energies of 0.03 eV (As; 248-300 Kj and 0.31 eV (P). The resistivity is suppressed in the presence of a magnetic field, with the greatest dp occurring at a magnetic transition similar to that found in other colossal magnetoresistive materials. The magnetoresistivity (MR) ratios (rho (H=0) - rho (H=5T))/rho (H 5T) at the magnetic transition are 1200 at 55 K (Eu14MnP11) and 2 at 74 K (Eu14MnAs11). Structural features as well as magnetic, electronic, and magnetotransport properties are presented and compared within the Eu(14)MnPn(11) series.

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