Optical spectroscopy study on pressure-induced phase transitions in the three-dimensional Dirac semimetal Cd3As2
Source abstract
Abstract
We report a room-temperature optical reflectivity study performed on [112]-oriented ${\mathrm{Cd}}3{\mathrm{As}}2$ single crystals over a broad energy range under external pressure up to 10 GPa. The abrupt drop in the band dispersion parameter ($z$ parameter) and the interruption of the gradual redshift of the band gap at $\ensuremath{\sim}4\phantom{\rule{0.28em}{0ex}}\mathrm{GPa}$ confirm the structural phase transition from a tetragonal to a monoclinic phase in this material. The pressure-induced increase in the overall optical conductivity at low energies and the continuous redshift of the high-energy bands indicate that the system evolves towards a topologically trivial metallic state, although a complete closing of the band gap could not be observed in the studied pressure range. Furthermore, a detailed investigation of the low-pressure regime suggests the possible existence of an intermediate state between 2 and 4 GPa, that might be a precursor of the structural phase transition or due to the lifted degeneracy of the Dirac nodes. Several optical parameters show yet another anomaly at 8 GPa where low-temperature superconductivity was found in an earlier study.
Source: openalex_inverted_index · Quality: baseline
Research context
OpenAlex topics: Topological Materials and Phenomena · Advanced Condensed Matter Physics · Electronic and Structural Properties of Oxides
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
References (29)
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1. 10.1103/PhysRevB.85.19532010.1103/PhysRevB.85.195320 ↗
2. 10.1103/PhysRevLett.108.14040510.1103/PhysRevLett.108.140405 ↗
3. 10.1103/PhysRevB.88.12542710.1103/PhysRevB.88.125427 ↗
4. 10.1080/00018732.2014.92710910.1080/00018732.2014.927109 ↗
5. 10.1038/ncomms478610.1038/ncomms4786 ↗
6. 10.1146/annurev-conmatphys-020911-12513810.1146/annurev-conmatphys-020911-125138 ↗
7. 10.1038/ncomms589810.1038/ncomms5898 ↗
8. 10.1103/PhysRevB.93.12120210.1103/PhysRevB.93.121202 ↗
9. 10.1103/PhysRevLett.117.13640110.1103/PhysRevLett.117.136401 ↗
10. 10.1103/PhysRevB.91.16513310.1103/PhysRevB.91.165133 ↗
11. 10.1038/npjquantmats.2016.1410.1038/npjquantmats.2016.14 ↗
12. 10.1103/PhysRevB.96.15520510.1103/PhysRevB.96.155205 ↗
13. 10.1038/srep1296610.1038/srep12966 ↗
14. 10.1063/1.113506510.1063/1.1135065 ↗
15. 10.1029/JB091iB05p0467310.1029/JB091iB05p04673 ↗
16. 10.1103/PhysRevB.74.16511810.1103/PhysRevB.74.165118 ↗
17. 10.1103/PhysRevLett.108.04660210.1103/PhysRevLett.108.046602 ↗
18. 10.1103/PhysRevB.87.12542510.1103/PhysRevB.87.125425 ↗
19. 10.1103/PhysRevB.87.23512110.1103/PhysRevB.87.235121 ↗
20. 10.1103/PhysRevB.92.07510710.1103/PhysRevB.92.075107 ↗
21. 10.1103/PhysRevLett.113.02760310.1103/PhysRevLett.113.027603 ↗
22. 10.1038/nmat399010.1038/nmat3990 ↗
23. 10.1038/nmat402310.1038/nmat4023 ↗
24. 10.1103/PhysRevB.89.24512110.1103/PhysRevB.89.245121 ↗
25. 10.1103/PhysRevB.93.08542610.1103/PhysRevB.93.085426 ↗
26. 10.1103/PhysRevB.93.08544210.1103/PhysRevB.93.085442 ↗
27. 10.1103/PhysRevB.94.08512110.1103/PhysRevB.94.085121 ↗
28. 10.1038/srep1985310.1038/srep19853 ↗
29. 10.1103/PhysRev.124.186610.1103/PhysRev.124.1866 ↗