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http://www.scirp.org/journal/PaperInformation.aspx?PaperID=52962#.VK3shMnQrzE
Author(s)
Adolfo Quiroz1,2, Elizabeth Chavira2, José Eduardo Espinosa1, Rodolfo Palomino-Merino1, Ernesto Esteban Marinero3, Masaya Nishioka4, Valentín García-Vázquez5
Affiliation(s)
1Facultad
de Ciencias Físico-Matemáticas, Postgrado en Física Aplicada,
Benemérita Universidad Autónoma Puebla, Ciudad Universitaria, Puebla,
México.
2Instituto de Investigaciones en Materiales, Universidad Nacional Autónoma de México, México, D.F., México.
3Purdue University, West Lafayette, IN, USA.
4Hitachi San José Research Center, San José, California, USA.
5Instituto de Física LRT, Benemérita Universidad Autónoma de Puebla, Puebla, México.
2Instituto de Investigaciones en Materiales, Universidad Nacional Autónoma de México, México, D.F., México.
3Purdue University, West Lafayette, IN, USA.
4Hitachi San José Research Center, San José, California, USA.
5Instituto de Física LRT, Benemérita Universidad Autónoma de Puebla, Puebla, México.
ABSTRACT
We present a study of their structure, morphology, electrical and magnetic properties on the (Ca1<span "="">–xSrx) RuO3 system for x
= 0.0, 0.07, 0.10, 0.15 and 1.0. The samples were prepared by the
solidstate reaction method in air at ambient pressure and heat in the
700℃ - 800℃ range for 48 h. By X-ray powder diffraction (XRD), we
determine a solid solution until x = 0.15. Scanning electron
microscopy (SEM) indicates that the particle size is 77 - 266 nm. The
resistance measurements, as a function of temperature measurements from 7
to 300 K the (Ca1<span "="">–xSrx) RuO3 system for x
= 0.0, 0.07, 0.10, 0.15 and 1.0 show a metallic behaviour. We can even
observe that the resistance of the samples is due to the partial
substitution of Sr2+ ions and Ru ion valence. Finally, the sample x = 0.07 has a magnetization applied high field to 10 K, whereas that to 300 K does not have a magnetization.
Cite this paper
References
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