Abstract
Many-body excitons in CrSBr are attracting intense interest in view of their highly anisotropic magneto-optical coupling and their potential for novel optical interfaces within spintronic and magnonic devices. Characterizing the orbital character and propagation of these electronic excitations is crucial for understanding and controlling their behavior; however, this information is challenging to access. High resolution resonant inelastic x-ray scattering is a momentum-resolved technique that can address these crucial questions. We present measurements collected at the Cr L3-edge which show a rich spectrum of excitations with a variety of spin-orbital characters. While most of these excitations appear to be localized, the dispersion of the lowest energy dark exciton indicates that it is able to propagate along both the a and b directions within the planes of the crystal. This two-dimensional character is surprising as it contrasts with electrical conductivity and the behavior of the bright exciton, both of which are strongly one dimensional. The discovery of this propagating dark exciton highlights an unusual coexistence of one- and two-dimensional electronic behaviors in CrSBr.
| Original language | English |
|---|---|
| Article number | 146503 |
| Journal | Physical Review Letters |
| Volume | 135 |
| Issue number | 14 |
| DOIs | |
| State | Published - Oct 3 2025 |
Funding
Work at Brookhaven and Harvard is supported by the Office of Basic Energy Sciences, Materials Sciences and Engineering Division, U.S. Department of Energy (DOE) under Contract No. DE-SC0012704. Work at the University of Tennessee (RIXS calculations and interpretation by model Hamiltonian calculations) was supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under Award No. DE-SC0022311. E.B. was supported by the United States Army Research Office (W911NF-23-1-0394). Synthesis work at Columbia University was supported by the Programmable Quantum Materials, an Energy Frontier Research Center funded by the U.S. Department of Energy (DOE), Office of Science, Basic Energy Sciences (BES), under Award No. DESC0019443. This research used ESRF beam line ID32 under proposal HC5030. Part of this research (T.B.) was conducted at the Center for Nanophase Materials Sciences, which is a DOE Office of Science User Facility. The work by J.W.V. is supported by the Quantum Science Center (QSC), a National Quantum Information Science Research Center of DOE. We also acknowledge resources made available through BNL/LDRD#19-013. This research used beamline 2-ID of the National Synchrotron Light Source II, a U.S. DOE Office of Science User Facility operated for the DOE Office of Science by Brookhaven National Laboratory under Contract No. DE-SC0012704. Work at Brookhaven and Harvard is supported by the Office of Basic Energy Sciences, Materials Sciences and Engineering Division, U.S. Department of Energy (DOE) under Contract No. DE-SC0012704. Work at the University of Tennessee (RIXS calculations and interpretation by model Hamiltonian calculations) was supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under Award No. DE-SC0022311. E. B. was supported by the United States Army Research Office (W911NF-23-1-0394). Synthesis work at Columbia University was supported by the Programmable Quantum Materials, an Energy Frontier Research Center funded by the U.S. Department of Energy (DOE), Office of Science, Basic Energy Sciences (BES), under Award No. DESC0019443. This research used ESRF beam line ID32 under proposal HC5030. Part of this research (T. B.) was conducted at the Center for Nanophase Materials Sciences, which is a DOE Office of Science User Facility. The work by J. W. V. is supported by the Quantum Science Center (QSC), a National Quantum Information Science Research Center of DOE. We also acknowledge resources made available through BNL/LDRD#19-013. This research used beamline 2-ID of the National Synchrotron Light Source II, a U.S. DOE Office of Science User Facility operated for the DOE Office of Science by Brookhaven National Laboratory under Contract No. DE-SC0012704.
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