1990
DOI: 10.1016/0304-8853(90)90689-n
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Magnetic properties of CrSBr

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Cited by 76 publications
(111 citation statements)
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“…The sharpness of the AF–FP transition along the b ‐axis confirms that it is the magnetic easy axis. [ 25 ] The saturation magnetic fields determined from the magnetization curves correlate well with H S extracted from the magnetoresistance data for each field direction. From the combined magnetotransport and magnetization measurements, we conclude that the electrical properties of CrSBr are strongly coupled to the magnetic order; the observed magnetotransport properties are a direct result of the layered antiferromagnetic structure of CrSBr.…”
Section: Figurementioning
confidence: 67%
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“…The sharpness of the AF–FP transition along the b ‐axis confirms that it is the magnetic easy axis. [ 25 ] The saturation magnetic fields determined from the magnetization curves correlate well with H S extracted from the magnetoresistance data for each field direction. From the combined magnetotransport and magnetization measurements, we conclude that the electrical properties of CrSBr are strongly coupled to the magnetic order; the observed magnetotransport properties are a direct result of the layered antiferromagnetic structure of CrSBr.…”
Section: Figurementioning
confidence: 67%
“…Along the b ‐axis, M sharply transitions from zero to the saturation magnetization, typical of a first order AF–FP spin‐flip transition (Figure 4B). [ 25,37 ] The M versus B curves along the a ‐ and c ‐axes (in‐plane intermediate and out‐of‐plane hard magnetic axes, respectively) exhibit a continuous increase of M from zero to the saturation magnetization, indicating that the spins are progressively canting to align with B (Figure 4A,C). The sharpness of the AF–FP transition along the b ‐axis confirms that it is the magnetic easy axis.…”
Section: Figurementioning
confidence: 99%
“…1c), which is an air-stable vdW semiconductor (bandgap of ~1.5 eV; see Supplementary Section 18 for transport measurements) with an interlayer AFM ordering up to a relatively high Néel temperature of T N ≈ 132 K (refs. [34][35][36][37] ). Furthermore, the antiferromagnetism promises ultrafast operations and robustness against external magnetic fields 38 and also is expected to be tunable by a gate electric field 35,39 .…”
Section: Electrical and Thermal Generation Of Spin Currents By Magnet...mentioning
confidence: 99%
“…[2,4] In this report, we demonstrate a versatile approach to engineer the structural landscape and the related spin textures in layered vdW magnets with singleatom precision. We conduct our study on the recently rediscovered vdW layered magnet CrSBr [31][32][33][34] that constitutes an ideal candidate due to its known amenability for intrinsic structural changes [32] and its highly promising electronic, optical and magnetic properties. [31][32][33][34][35][36][37] CrSBr is an air-stable ferromagnetic (FM) insulator in the monolayer limit with a direct band gap of ∼ 1.6 eV [33][34][35] hosting tightly bound magneto-excitons.…”
mentioning
confidence: 99%
“…We conduct our study on the recently rediscovered vdW layered magnet CrSBr [31][32][33][34] that constitutes an ideal candidate due to its known amenability for intrinsic structural changes [32] and its highly promising electronic, optical and magnetic properties. [31][32][33][34][35][36][37] CrSBr is an air-stable ferromagnetic (FM) insulator in the monolayer limit with a direct band gap of ∼ 1.6 eV [33][34][35] hosting tightly bound magneto-excitons. [37] The magnetic easy axis is in-plane with an antiferromagnetic (AFM) interlayer coupling in the bulk with a Néel temperature of T N = 132 K [32,36] and a recently suggested intermediate soft magnetic phase up to 160 K. [35] The combination of these properties and the crystal stability makes CrSBr ideal for nanoscale structural modification, and hence the creation of spin textures with atomic resolution, a key requirement for building advanced spintronic and magneto-electric devices.…”
mentioning
confidence: 99%