2014
DOI: 10.1103/physrevb.89.121114
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Photoinduced sign inversion of the anomalous Hall effect in EuO thin films

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Cited by 8 publications
(4 citation statements)
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“…The classical ferromagnetic semiconductor EuO [118,119] is one of the leading candidates hosting skyrmionic structures. As shown in figure 6(a), topological Hall resistivity ρ THE has been observed as a sharp peak in the magnetization process in EuO, in addition to the conventional anomalous Hall resistivity ρ AHE proportional to magnetization [120][121][122]. The ρ THE peak appears only in films thinner than t = 200 nm.…”
Section: Topological Spin Structures In Oxide Filmsmentioning
confidence: 87%
“…The classical ferromagnetic semiconductor EuO [118,119] is one of the leading candidates hosting skyrmionic structures. As shown in figure 6(a), topological Hall resistivity ρ THE has been observed as a sharp peak in the magnetization process in EuO, in addition to the conventional anomalous Hall resistivity ρ AHE proportional to magnetization [120][121][122]. The ρ THE peak appears only in films thinner than t = 200 nm.…”
Section: Topological Spin Structures In Oxide Filmsmentioning
confidence: 87%
“…AHE is known to increase with carrier concentration (n) [27]. Photoionization experiments, elevating n to about 4 • 10 19 cm −3 (30% increase) [31], indeed change the anomalous Hall conductivity σ AH from 0.2 S•cm −1 to about 1 S•cm −1 . Remarkably, at a critical value of longitudinal conductivity σ xx ≈ 100 S•cm −1 , σ AH reverses its sign from negative to positive with respect to magnetic field.…”
Section: Introductionmentioning
confidence: 93%
“…It is suggested [33] that carrier concentrations in EuO exceeding 5 • 10 −19 cm −3 can be reached only by chemical doping with rare-earth trivalent metals. Also, oxygen-deficient EuO employed in AHE experiments [30][31][32][33] is synthesized using pulsed laser deposition-a technique that can hardly control dopant incorporation-leading to an uncontrolled amount and distribution of defects. Here we report the successful synthesis of Gd-doped EuO epitaxial films within heterostructures SiO/Eu 1−x Gd x O/ EuO/Si employing the full potential of molecular beam epitaxy to control the doping.…”
Section: Introductionmentioning
confidence: 99%
“…The interest in EuO has seen a considerable upswing recently due to its potential as a spintronics material. For example, EuO devices were employed to for spin filtering [9][10][11][12], the interface between EuO and GdN is expected to produce a band inversion and a nonzero Chern number [13], a giant spin-phonon coupling has been reported [14], it has been suggested that a CdO/EuO superlattice is a Weyl semimetal [15], and the Hall effect of EuO thin films has been observed [16,17]. Efforts to increase the Curie temperature via doping and alloying of EuO have also seen a resurgency: Curie temperatures up to 134 K in single crystals and even higher in thin films have been achieved [18][19][20][21][22][23][24][25][26][27].…”
Section: Introductionmentioning
confidence: 99%