Abstract
We report the results of a temperature-dependent reflection spectroscopy study, across a wide energy range (∼0.01 to 3 eV), of unsubstituted and 40% Zn substituted for Co, for the transition-metal phosphorus trichalcogenide, Co2P2S6. We observe a transition from a paramagnetic to antiferromagnetic state with a Néel temperature at TN∼120 K that is completely suppressed in Zn-substituted samples. At 300 K we identify four narrow (∼1 meV) infrared active phonon modes while at 70 K (below TN) we observe that the low-energy phonons, dominated by Co motion, resolve into two modes. These low-energy modes are asymmetric, indicating coupling to a broad electronic continuum. We also report a broad (∼30 meV) low-temperature infrared absorption band that appears near TN that we suggest is determined by a multiphonon-assisted 2-magnon absorption process. At 300 K in higher-energy spectra, we observe considerable absorption starting from 0.20±0.02 eV which we associate with inter-Co2+ ion 3d transitions. At temperatures below TN the number of electronic absorption bands increases from 4 to 6, indicating a lowering of the symmetry around the Co2+ ions. On substituting 40% Zn for Co, the antiferromagnetic transition is suppressed along with temperature-dependent changes in the phonon and electronic spectra. The temperature-dependent spectral changes indicate strongly correlated behavior between the infrared active lattice vibrations, the electronic excitations, and magnetism in unsubstituted Co2P2S6.
| Original language | English |
|---|---|
| Article number | 165142 |
| Journal | Physical Review B |
| Volume | 109 |
| Issue number | 16 |
| DOIs | |
| State | Published - Apr 15 2024 |
Funding
This research was supported by a University Research Fund grant from Victoria University of Wellington. The MacDiarmid Institute for Advanced Materials and Nanotechnology is supported under the New Zealand Centres of Research Excellence Programme. This research was additionally supported by the Air Force Office of Scientific Research (AFOSR), Grant No. LRIR23RXCOR003, and AOARD-NSTC, Grant No. F4GGA21207H002. We also acknowledge support from the National Research Council's Senior NRC Associateship program sponsored by the National Academies of Science, Engineering, and Medicine and administered by the AFRL Sensors Directorate. Low-temperature x-ray-diffraction measurements (M.A.M.) were supported by the U.S. Department of Energy, Office of Science, Basic Energy Sciences, Materials Sciences and Engineering Division.
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