Abstract
We present the magnetic behavior and resulting transport properties of TaSe2 when intercalated by magnetically active cobalt cations. Acting as the layered host, TaSe2 is a transition metal dichalcogenide (TMD) that adopts the 2H-polytype. We find through our single crystal and powder diffraction studies that we can prepare the stoichiometry Co1/4TaSe2, which crystallizes in the centrosymmetric space group P63/mmc. From magnetic susceptibility and x-ray photoelectron spectroscopy measurements, we find a transition consistent with antiferromagnetic order below the temperature TN=173K and Co2+ in the high-spin state. Neutron powder diffraction and specific heat measurements, however, point to a much smaller than anticipated ordered moment in this sample. From the neutron results, the magnetic structure can be described as an A-type antiferromagnet with an ordered moment size of 1.35(11) μB per Co cation. The direction of the moments is all long the c axis, which is consistent with the magnetization and susceptibility studies showing this direction to be the easy axis. Interestingly, we find that a weak and subtle ferromagnetic component appears to exist along the ab plane of the Co1/4TaSe2 crystals. We place the results of this work in the context of other magnetic-ion intercalated TMDs, especially those of Ta and Nb.
| Original language | English |
|---|---|
| Article number | 144420 |
| Journal | Physical Review B |
| Volume | 110 |
| Issue number | 14 |
| DOIs | |
| State | Published - Oct 1 2024 |
Funding
The authors thank the U.S. Department of Energy (DOE), Office of Science (Grant No. DE-SC0016434), for financial support. Use of the Spallation Neutron Source (POWGEN experiment IPTS-31862) at Oak Ridge National Laboratory was supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under Contract No. DE-AC02-06CH11357. Measurements were performed with the support of the National Science Foundation (NSF-DMR 2105191). We thank Harikrishnan S. Nair for the discussions. We also acknowledge support from the Quantum Materials Center. This work has been supported in part by the X-ray Crystallographic Center at The University of Maryland.
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