2009
DOI: 10.1016/j.jmmm.2009.01.032
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Magnetic and magneto-transport properties of double perovskite Ba2−xSrxFeMoO6 system

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Cited by 30 publications
(12 citation statements)
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“…The significant decrease of the saturation magnetic moment with x might be attributed to the increase of the anti-site disorder defects [22,23] or magnetic dilution due to the substitution of Cr for Fe. The values of S for pure compounds are in good agreement of those values reported in literatures [14,19]. It is worth noting that the observed value of the saturation magnetic moment for Ba 2 FeMoO 6 double perovskite lies slightly below the theoretical value of 4 B /f.u.…”
Section: Magnetic Propertiessupporting
confidence: 90%
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“…The significant decrease of the saturation magnetic moment with x might be attributed to the increase of the anti-site disorder defects [22,23] or magnetic dilution due to the substitution of Cr for Fe. The values of S for pure compounds are in good agreement of those values reported in literatures [14,19]. It is worth noting that the observed value of the saturation magnetic moment for Ba 2 FeMoO 6 double perovskite lies slightly below the theoretical value of 4 B /f.u.…”
Section: Magnetic Propertiessupporting
confidence: 90%
“…The results show a continuous decrease in the lattice constant with increasing Cr content in the samples (a = 8.061 Å for Ba 2 FeMoO 6 and a = 8.013 Å for Ba 2 CrMoO 6 ) which is obvious due to smaller ionic radius of Cr 3+ (0.615 Å) compared to ionic radius of Fe 3+ (0.645 Å). The lattice parameter values of parent compounds are in good agreement with lattice parameters of Ba 2 FeMoO 6 and Ba 2 CrMoO 6 reported in literatures [16,19].…”
Section: Structural Characterizationsupporting
confidence: 88%
“…As a subclass of perovskite-type oxides ABO 3 , the double perovskite-type oxide AA BB O 6 have attracted more and more attentions as magnetic materials [1] , superconducting materials [2] , and catalytic materials [3][4][5] , due to its unique structure and multiple properties. In the double perovskite-type A A B B O 6 structure, B −O 6 and B −O 6 octahedras are arranged alternately by the way of corner-sharing with A cations occupy the voids between the octahedral [6] .…”
Section: Introductionmentioning
confidence: 99%
“…A 2 FeMoO 6 (A = Sr, Ba) [2][3][4] and many of its structural materials [5,6], have attracted considerable scientific and technological interest in recent years due to its reported room temperature (415 • C for Sr 2 FeMoO 6 and 330 • C for Ba 2 FeMoO 6 ) low-field magneto-resistance [7,8]. This property, related to the variation of electric resistivity when a magnetic field is applied, is a consequence of the half-metallic character of the double perovskite, and can also been attributed to spin dependent scattering of charge carriers at grain boundaries extended to inter grain-tunneling effect.…”
Section: Introductionmentioning
confidence: 99%