2021
DOI: 10.1103/physrevb.104.144416
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Triaxial magnetic anisotropy in the two-dimensional ferromagnetic semiconductor CrSBr

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Cited by 79 publications
(108 citation statements)
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“…Rather uncommonly, the relatively large low-temperature conductivity -which confirms the presence of sizable non-intentional doping-coexists with a bright fluorescence observed in photoluminescence experiments (see Figure 1e) [24]. Additionally, the same band structure calculations (see Figure 1b) predicting a large bandwidth also show an extremely pronounced anisotropy: the bandwidth is about 1.5 eV in the Γ − Y (which corresponds to the crystallographic b-axis), but nearly vanishes in the perpendicular Γ − X direction (i.e., in the a-direction) [24,25]. Even though this prediction is somewhat surprising, because no obvious pronounced anisotropy can be identified in the atomic structure of the material (see Figure 1a), indications of anisotropy (see Figure 1e) were indeed found when measuring the photoluminescence polar- ization dependence [24].…”
Section: Introductionsupporting
confidence: 53%
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“…Rather uncommonly, the relatively large low-temperature conductivity -which confirms the presence of sizable non-intentional doping-coexists with a bright fluorescence observed in photoluminescence experiments (see Figure 1e) [24]. Additionally, the same band structure calculations (see Figure 1b) predicting a large bandwidth also show an extremely pronounced anisotropy: the bandwidth is about 1.5 eV in the Γ − Y (which corresponds to the crystallographic b-axis), but nearly vanishes in the perpendicular Γ − X direction (i.e., in the a-direction) [24,25]. Even though this prediction is somewhat surprising, because no obvious pronounced anisotropy can be identified in the atomic structure of the material (see Figure 1a), indications of anisotropy (see Figure 1e) were indeed found when measuring the photoluminescence polar- ization dependence [24].…”
Section: Introductionsupporting
confidence: 53%
“…CrSBr has been recently identified as an extremely interesting 2D magnetic semiconductor, rather unique because the width of its bands is approximately 1.5 eV or larger, i.e., 50-100 times larger than that of other semiconducting 2D magnetic materials that have been recently studied [7,24,25]. Earlier work has mainly focused on the magnetic properties of the material, exploiting the fact that the large bandwidth results in a conductivity that is also sufficiently large to remain measurable at low temperature, well below the magnetic transition temperature.…”
Section: Discussionmentioning
confidence: 99%
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“…Furthermore, in such mixed-anion compounds 21 , the relative arrangement of the heavy halides allows for a specific modification of the magnetic interactions by a targeted control of the magnetic anisotropy. In this line, the antiferromagnetic (AFM), mixed-anion, van der Waals material CrSBr 22 stands out by combining a sizeable direct band gap of ∆E ≈ 1.8 eV with an exceptionally large band-width 23,24 , and thus an expected high carrier mobility 25 . Furthermore, CrSBr exhibits a substantial air-stability and a high magnetic critical temperature of T N ≈ 133 K in bulk, predicted to be even higher in the monolayer [24][25][26] .…”
Section: Introductionmentioning
confidence: 99%
“…In this line, the antiferromagnetic (AFM), mixed-anion, van der Waals material CrSBr 22 stands out by combining a sizeable direct band gap of ∆E ≈ 1.8 eV with an exceptionally large band-width 23,24 , and thus an expected high carrier mobility 25 . Furthermore, CrSBr exhibits a substantial air-stability and a high magnetic critical temperature of T N ≈ 133 K in bulk, predicted to be even higher in the monolayer [24][25][26] . A substantial magnetoresistance has been indeed demonstrated below the ordering temperature 27 .…”
Section: Introductionmentioning
confidence: 99%