2003
DOI: 10.1103/physrevb.67.014422
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Electronic properties of 4-nm FePt particles

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Cited by 106 publications
(98 citation statements)
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“…[28] The coercivity of composites reduced at 750°C is also lower as compared to isolated FePt nanoparticles but comparable to FePt silica coreshell structures reported by Yu et al [29] For samples synthesized by the oxidation method, the magnetization at H = 4 kOe is significantly lower at 300 K than at 2 K, while for samples prepared via direct reduction the temperature dependence of the magnetization was not pronounced. and B h = 31.2(1) T at 4.2 K. In contrast to the line broadening effects between 250 and 185 K observed for 4 nm FePt particles, [30,31] we already observe hyperfine field splitting at room temperature, in agreement with the magnetization data taken at 300 K. The observed hyperfine field slightly increases from room temperature to 4.2 K with values similar to those for the 4 nm FePt nanoparticles. [30,31] Summarizing, we have demonstrated efficient generation of FePt nanoparticles in an ordered mesoporous oxide and subsequent transformation of the cubic FePt nanoparticles into fct-FePt.…”
supporting
confidence: 83%
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“…[28] The coercivity of composites reduced at 750°C is also lower as compared to isolated FePt nanoparticles but comparable to FePt silica coreshell structures reported by Yu et al [29] For samples synthesized by the oxidation method, the magnetization at H = 4 kOe is significantly lower at 300 K than at 2 K, while for samples prepared via direct reduction the temperature dependence of the magnetization was not pronounced. and B h = 31.2(1) T at 4.2 K. In contrast to the line broadening effects between 250 and 185 K observed for 4 nm FePt particles, [30,31] we already observe hyperfine field splitting at room temperature, in agreement with the magnetization data taken at 300 K. The observed hyperfine field slightly increases from room temperature to 4.2 K with values similar to those for the 4 nm FePt nanoparticles. [30,31] Summarizing, we have demonstrated efficient generation of FePt nanoparticles in an ordered mesoporous oxide and subsequent transformation of the cubic FePt nanoparticles into fct-FePt.…”
supporting
confidence: 83%
“…and B h = 31.2(1) T at 4.2 K. In contrast to the line broadening effects between 250 and 185 K observed for 4 nm FePt particles, [30,31] we already observe hyperfine field splitting at room temperature, in agreement with the magnetization data taken at 300 K. The observed hyperfine field slightly increases from room temperature to 4.2 K with values similar to those for the 4 nm FePt nanoparticles. [30,31] Summarizing, we have demonstrated efficient generation of FePt nanoparticles in an ordered mesoporous oxide and subsequent transformation of the cubic FePt nanoparticles into fct-FePt. The mesoporous matrix with well defined pore size COMMUNICATION 3024 www.advmat.de allows to control the particle diameter and hinders sintering and aggregation during the thermally induced phase transformation.…”
supporting
confidence: 83%
“…4,6,7 Due to the reported M s values that are much lower than expected for a fcc FePt bulk at 5 K, it is attributed to the presence of the nonmagnetic Fe shell. Nevertheless, the mechanism by which M s is too low is not completely understood.…”
Section: Discussionmentioning
confidence: 93%
“…Recent works [3][4][5][6][7] have proved that the synthesis by a high-boiling coordinating solvent method gives place to a core-shell structure of the FePt NPs. Delalande et al 3 have proposed that FePt NPs have a Pt rich core and a Fe rich shell due to the different nucleation kinetics of Pt and Fe: Pt nucleates faster and easier than Fe.…”
Section: Discussionmentioning
confidence: 99%
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