2013
DOI: 10.1021/jz401115q
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Room-Temperature Ferromagnetism in Reduced Rutile TiO2−δ Nanoparticles

Abstract: We report a synthesis method to stabilize TiO 2 rutile nanoparticles (around 10 nm) and keep the particle size when reduced down to TiO 1.84 . TiO 2−δ nanoparticles exhibit room-temperature ferromagnetism that becomes stronger for TiO 1.84 . The reduction mechanism to stabilize Magneli phases excludes a relevant influence of oxygen vacancies in the modification of the magnetic properties. The arrangement of Ti 3+ could give rise to hopping of the single 3d electron inducing local ferromagnetic-like behavior.

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Cited by 56 publications
(40 citation statements)
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References 29 publications
(56 reference statements)
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“…The modulated AFM order transformed to a collinear FM order in a magnetic field above 21 kOe at 5 K. For example, the difference between the zero-field and non-zero-field ND profiles clearly revealed the presence of FM order (Figure 6a), which gradually developed with increasing magnetic field (Figure 6b). Figure 6c shows the applied magnetic field dependence of the magnetic peak intensity at 2θ = 30, which indicates The magnetic moments in the FM state at 5 K were estimated to be 2.13 (8) (Figure 3b), although the ND analysis yields approximately 3 µB/f.u. in total.…”
Section: Resultsmentioning
confidence: 98%
“…The modulated AFM order transformed to a collinear FM order in a magnetic field above 21 kOe at 5 K. For example, the difference between the zero-field and non-zero-field ND profiles clearly revealed the presence of FM order (Figure 6a), which gradually developed with increasing magnetic field (Figure 6b). Figure 6c shows the applied magnetic field dependence of the magnetic peak intensity at 2θ = 30, which indicates The magnetic moments in the FM state at 5 K were estimated to be 2.13 (8) (Figure 3b), although the ND analysis yields approximately 3 µB/f.u. in total.…”
Section: Resultsmentioning
confidence: 98%
“…This behavior is also found in the temperature dependence of the high field magnetization (applied magnetic field, µ 0 H = 6 T). The coexistence of both contributions has been reported in other doped and oxygen defective nanostructures [23], where the nearly independent magnetization is ascribed to the induced ferromagnetic component in the semiconductor. Finally, it should be outlined that all the samples display a certain splitting in the Zero Field Cool (ZFC)-Field Cool (FC) magnetization curves.…”
Section: Resultsmentioning
confidence: 65%
“…The main disadvantages of this strategy are crystal growth and agglomeration caused by the high temperatures required for reduction of the stable Ti 4+ to Ti 3+ . One of our previous articles evidenced that average particle size can be kept below 50 nm, particles ranging 5–10 nm can even be found, when a very small amount of material is reduced under strict control in a Cahn electrobalance. It allowed us to discuss the magnetic properties, room temperature ferromagnetism, of nanostructured Magnéli phases which were attributed to the presence of anionic vacancies in a previous article, and we evidence that this peculiar behavior was actually caused by the presence of Ti 3+ in the CS planes.…”
Section: Synthesis and Propertiesmentioning
confidence: 99%