2022
DOI: 10.1038/s41586-022-05024-1
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Exciton-coupled coherent magnons in a 2D semiconductor

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Cited by 79 publications
(78 citation statements)
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“…This lack of observable gap evidences highly isotropic magnetism, as one expects for S = 3/2 Cr 3 + . This comports with density functional theory predictions [ 15 ] and recent photon measurements finding Q = 0 magnon gaps of 0.102(3) and 0.141(4) meV, [ 16 ] as well as magnetization measurements finding a maximum anisotropy of 0.144 μeV$\rm \mu eV$ at 2 K ( c ‐axis compared to b ) in CrSBr (see Supporting Information [ 17 ] ): too small to be resolved in this experiment.…”
Section: Results and Analysissupporting
confidence: 89%
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“…This lack of observable gap evidences highly isotropic magnetism, as one expects for S = 3/2 Cr 3 + . This comports with density functional theory predictions [ 15 ] and recent photon measurements finding Q = 0 magnon gaps of 0.102(3) and 0.141(4) meV, [ 16 ] as well as magnetization measurements finding a maximum anisotropy of 0.144 μeV$\rm \mu eV$ at 2 K ( c ‐axis compared to b ) in CrSBr (see Supporting Information [ 17 ] ): too small to be resolved in this experiment.…”
Section: Results and Analysissupporting
confidence: 89%
“…This is consistent with the photon excitation study in ref. [16] which finds an interlayer exchange <0.01 meV, as well as density functional calculations in ref. [18] which finds a CrSBr interlayer magnetic interaction three orders of magnitude weaker than the in‐plane interactions.…”
Section: Results and Analysissupporting
confidence: 57%
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“…The van der Waals (vdW) antiferromagnets, a new class of exfoliatable magnetic materials, provide opportunities for future memory, logic, and communication devices because their magnetic properties are highly tunable, for example, by applied electric fields , or strain, they can possess long-lived magnons, and they can be straightforwardly integrated within complex heterostructures by mechanical assembly. , The strength of exchange coupling between vdW layers is typically much weaker than the direct exchange or superexchange coupling in ordinary three-dimensional crystal antiferromagnets. This weak interlayer exchange yields antiferromagnetic resonances in the gigahertz range, rather than the terahertz range that is more typical for antiferromagnets. The resonance modes in vdW antiferromagnets can therefore be addressed and controlled with conventional microwave electronics.…”
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confidence: 99%