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               <dc:title>Magnetic transitions in Pr2NiO4 single crystal</dc:title>
               <dc:creator>Obradors, Xavier</dc:creator>
               <dc:creator>Martínez Perea, Benjamin</dc:creator>
               <dc:creator>Batlle Gelabert, Xavier</dc:creator>
               <dc:creator>Rodríguez Carvajal, Juan</dc:creator>
               <dc:creator>Fernández-Diaz, M. T.</dc:creator>
               <dc:creator>Martínez, J. L.</dc:creator>
               <dc:creator>Odier, P.</dc:creator>
               <dc:subject>Propietats magnètiques</dc:subject>
               <dc:subject>Anisotropia</dc:subject>
               <dc:subject>Ferromagnetisme</dc:subject>
               <dc:subject>Spin (Física nuclear)</dc:subject>
               <dc:subject>Cristal·lografia</dc:subject>
               <dc:subject>Matèria condensada</dc:subject>
               <dc:subject>Magnetic properties</dc:subject>
               <dc:subject>Anisotropy</dc:subject>
               <dc:subject>Ferromagnetism</dc:subject>
               <dc:subject>Nuclear spin</dc:subject>
               <dc:subject>Cristallography</dc:subject>
               <dc:subject>Condensed matter</dc:subject>
               <dc:description>The magnetic properties of a stoichiometric Pr2NiO4 single crystal have been examined by means of the temperature dependence of the complex ac susceptibility and the isothermal magnetization in fields up to 200 kOe at T=4.2 K. Three separate phases have been identified and their anisotropic character has been analyzed. A collinear antiferromagnetic phase appears first between TN = 325 K and Tc1 = 115 K, where the Pr ions are polarized by an internal magnetic field. At Tc1 a first modification of the magnetic structure occurs in parallel with a structural phase transition (Bmab to P42/ncm). This magnetic transition has a first‐order character and involves both the out‐of‐plane and the in‐plane spin components (magnetic modes gx and gxcyfz, respectively). A second magnetic transition having also a first‐order character is also clearly identified at Tc2 = 90 K which corresponds to a spin reorientation process (gxcyfz to cxgyaz magnetic modes). It should be noted as well that the out‐of‐phase component of χac shows a peak around 30 K which reflects the coexistence of both magnetic configurations in a wide temperature interval. Finally, two field‐induced transitions have been observed at 4.2 K when the field is directed along the c axis. We propose that the high‐field anomaly arises from a metamagnetic transition of the weak ferromagnetic component, similarly to La2CuO4.</dc:description>
               <dc:date>2012-02-16T08:49:44Z</dc:date>
               <dc:date>2012-02-16T08:49:44Z</dc:date>
               <dc:date>1991</dc:date>
               <dc:type>info:eu-repo/semantics/article</dc:type>
               <dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
               <dc:relation>Reproducció del document publicat a:  http://dx.doi.org/10.1063/1.349958</dc:relation>
               <dc:relation>Journal of Applied Physics, 1991, vol. 70, núm. 10, p. 6329-6331</dc:relation>
               <dc:relation>http://dx.doi.org/10.1063/1.349958</dc:relation>
               <dc:rights>(c) American Institute of Physics, 1991</dc:rights>
               <dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
               <dc:publisher>American Institute of Physics</dc:publisher>
               <dc:source>Articles publicats en revistes (Física de la Matèria Condensada)</dc:source>
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