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2016
DOI: 10.1063/1.4961592
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Magnetic microstructure and magnetic properties of uniaxial itinerant ferromagnet Fe3GeTe2

Abstract: Magnetic force microscopy was used to observe the magnetic microstructure of Fe3GeTe2 at 4 K on the (001) surface. The surface magnetic structure consists of a two-phase domain branching pattern that is characteristic for highly uniaxial magnets in the plane perpendicular to the magnetic easy axis. The average surface magnetic domain width Ds = 1.3 μm determined from this pattern, in combination with intrinsic properties calculated from bulk magnetization data (the saturation magnetization Ms = 376 emu/cm3 and… Show more

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Cited by 113 publications
(119 citation statements)
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“…Second, it is predicted to be an itinerant ferromagnet with a relatively high-Curie temperature around 220 K. 26 Essentially, this becomes a very important figure of merit for spin-based technology architecture. Third, the anisotropy energy of Fe 3 GeTe 2 around 10 7 erg/cm 3 determined by magnetic force microscope 36 is much larger than that of CrGeTe 3 with 10 5 erg/cm 3 measured with FMR, 17 which is critical for magnetic tunnel junctions and magnetic random access memory devices. All of them require a large difference between anisotropy energy and thermal activation energy k B T for stable storage.…”
Section: Introductionmentioning
confidence: 86%
“…Second, it is predicted to be an itinerant ferromagnet with a relatively high-Curie temperature around 220 K. 26 Essentially, this becomes a very important figure of merit for spin-based technology architecture. Third, the anisotropy energy of Fe 3 GeTe 2 around 10 7 erg/cm 3 determined by magnetic force microscope 36 is much larger than that of CrGeTe 3 with 10 5 erg/cm 3 measured with FMR, 17 which is critical for magnetic tunnel junctions and magnetic random access memory devices. All of them require a large difference between anisotropy energy and thermal activation energy k B T for stable storage.…”
Section: Introductionmentioning
confidence: 86%
“…A possible explanation for this behavior is the formation of domain structures that are unresolvable through our optical measurements. Bulk crystal FGT exhibits stripy and bubble-like domains 10,23,24 . On the other hand, Co/Pt multilayer films with low disorder 25 show similar hysteresis loops to those in Fig.…”
Section: Main Textmentioning
confidence: 99%
“…The Fe(1) site is fully occupied, whereas a deficiency of Fe on the Fe(2) site easily forms during sample growth. Different forms of Fe 3 GeTe 2 have been grown, such as polycrystal, single crystal,35h,37,84,85 and thin film, where the lattice parameters and magnetic properties strongly depend on the Fe concentration and the growth conditions. Basically, additional nominal Fe doping decreases the lattice constant c while increasing the constant a .…”
Section: Bulk Counterparts Of Intrinsic Vdw Magnetsmentioning
confidence: 99%
“…The Fe 3 GeTe 2 single crystal exhibits strong out‐of‐plane easy magnetization anisotropy (Figure b) with a T C of ≈223 K. Due to its low‐symmetry crystal structure, the uniaxial magnetocrystalline anisotropy constant K u of Fe 3 GeTe 2 is calculated to be as large as ≈10 7 erg cm −3 . Magnetic studies suggest that Fe 3 GeTe 2 is a strongly correlated itinerant ferromagnet with highly anisotropic magnetic behavior.…”
Section: Bulk Counterparts Of Intrinsic Vdw Magnetsmentioning
confidence: 99%