journal article·2025-03-11Open access

Pressure-Driven Polar Orthorhombic to Tetragonal Phase Transition in Hafnia at Room Temperature

Janice L. Musfeldt, Sobhit Singh, Kevin A. Smith, Xianghan Xu, Sang-Wook Cheong, Zhenxian Liu, David Vanderbilt, Karin M. Rabe

Chemistry of Materials· Volume 37· Issue 5

Abstract

High Resolution Image Download MS PowerPoint Slide Oxides are legendary for their complex energy landscapes, sensitivity to external stimuli, and property control through chemical substitution. Of these, the binary oxide HfO 2 is one of the most fascinating because of the extraordinary number competing phases and opportunities to stabilize unique and useful properties. In this work, we combined synchrotron-based infrared absorbance and Raman scattering spectroscopies with diamond anvil cell techniques and first-principles calculations to explore the properties of polar orthorhombic hafnia (chemical formula HfO 2: x Y, where x = 12%) under pressure. Compression drives this system to the tetragonal form above 22 GPa─quite different from the more conventional phase diagram derived from pressurization of monoclinic HfO 2 where the tetragonal phase resides at elevated temperatures. In addition to evidence for a complex energy landscape, we unveil a wide coexistence region, order-of-magnitude differences in phonon lifetimes, and an A 1 g symmetry phonon in the tetragonal phase with a negative mode Grüneisen parameter that drives the system toward the cubic phase. Similar pressure pathways may connect other metastable phases in this family of materials.
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Research context

OpenAlex topics: Ferroelectric and Negative Capacitance Devices · Semiconductor materials and devices · Electronic and Structural Properties of Oxides

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

Affiliations

Department of Chemistry

University of Tennessee

Department of Physics and Astronomy

Department of Mechanical Engineering

University of Rochester

Materials Science Program

Rutgers University

Rutgers Center for Emergent Materials

Department of Physics

University of Illinois Chicago

Funding

Rutgers, The State University of New Jersey · Gordon and Betty Moore Foundation · Basic Energy Sciences · Advanced Research Projects Agency - Energy · University of Tennessee · Office of Naval Research · University of Rochester · National Science Foundation · Division of Materials Research

References (56)

Show source-provided references
1. 10.1063/5.003528110.1063/5.0035281 ↗
2. 10.1038/s41578-022-00431-210.1038/s41578-022-00431-2 ↗
3. 10.1038/s41563-023-01507-210.1038/s41563-023-01507-2 ↗
4. 10.1063/1.363405210.1063/1.3634052 ↗
5. 10.1038/358136a010.1038/358136a0 ↗
6. 10.1126/science.aba006710.1126/science.aba0067 ↗
7. 10.1557/JMR.1996.035010.1557/JMR.1996.0350 ↗
8. 10.1038/s41467-020-15159-210.1038/s41467-020-15159-2 ↗
9. 10.1021/acsaelm.1c0011010.1021/acsaelm.1c00110 ↗
10. 10.1038/s41586-022-04425-610.1038/s41586-022-04425-6 ↗
11. 10.1038/s41928-023-00959-310.1038/s41928-023-00959-3 ↗
12. 10.1103/PhysRevLett.125.25760310.1103/PhysRevLett.125.257603 ↗
13. 10.1103/PhysRevB.102.21410810.1103/PhysRevB.102.214108 ↗
14. 10.1039/C9CP01880H10.1039/C9CP01880H ↗
15. 10.1063/5.014806810.1063/5.0148068 ↗
16. 10.1021/acsaelm.4c0107110.1021/acsaelm.4c01071 ↗
17. 10.1103/PhysRevB.90.14010310.1103/PhysRevB.90.140103 ↗
18. 10.1103/PhysRevMaterials.5.06440510.1103/PhysRevMaterials.5.064405 ↗
19. Qi, Y. Polarization switching mechanism in HfO2 from first-principles lattice mode analysis. arXiv preprint: 2108.12538 (2021).
20. 10.1126/sciadv.add595310.1126/sciadv.add5953 ↗
21. 10.1103/PhysRevLett.131.25680110.1103/PhysRevLett.131.256801 ↗
22. 10.1103/PhysRevLett.131.22680210.1103/PhysRevLett.131.226802 ↗
23. 10.1016/j.mtphys.2023.10106410.1016/j.mtphys.2023.101064 ↗
24. 10.1038/s43246-023-00421-z10.1038/s43246-023-00421-z ↗
25. 10.1103/PhysRevB.108.09410910.1103/PhysRevB.108.094109 ↗
26. 10.1002/aelm.20220026510.1002/aelm.202200265 ↗
27. 10.1111/j.1151-2916.2001.tb00843.x10.1111/j.1151-2916.2001.tb00843.x ↗
28. 10.1134/S106378340710025310.1134/S1063783407100253 ↗
29. 10.1038/s41535-022-00436-810.1038/s41535-022-00436-8 ↗
30. 10.1002/pssr.20210058910.1002/pssr.202100589 ↗
31. 10.1021/acsaelm.4c0013410.1021/acsaelm.4c00134 ↗
32. 10.1038/s41563-020-00897-x10.1038/s41563-020-00897-x ↗
33. 10.1021/acsomega.9b0058010.1021/acsomega.9b00580 ↗
34. 10.1021/acsaelm.1c0067210.1021/acsaelm.1c00672 ↗
35. 10.1103/PhysRevMaterials.7.04441210.1103/PhysRevMaterials.7.044412 ↗
36. 10.1073/pnas.231257112110.1073/pnas.2312571121 ↗
37. 10.1002/admt.20180011110.1002/admt.201800111 ↗
38. 10.1111/j.1151-2916.1992.tb04149.x10.1111/j.1151-2916.1992.tb04149.x ↗
39. 10.1103/PhysRevB.48.920510.1103/PhysRevB.48.9205 ↗
40. 10.1103/PhysRevB.48.9310.1103/PhysRevB.48.93 ↗
41. 10.1103/PhysRevB.59.846710.1103/PhysRevB.59.8467 ↗
42. 10.1103/PhysRevB.82.14410610.1103/PhysRevB.82.144106 ↗
43. 10.1103/PhysRevB.90.06411110.1103/PhysRevB.90.064111 ↗
44. 10.1016/j.matpr.2016.09.01310.1016/j.matpr.2016.09.013 ↗
45. 10.1002/aelm.20200072810.1002/aelm.202000728 ↗
46. 10.1063/1.32527710.1063/1.325277 ↗
47. 10.1103/PhysRevB.54.1116910.1103/PhysRevB.54.11169 ↗
48. 10.1016/0927-0256(96)00008-010.1016/0927-0256(96)00008-0 ↗
49. 10.1103/PhysRevB.59.175810.1103/PhysRevB.59.1758 ↗
50. 10.1103/PhysRevB.50.1795310.1103/PhysRevB.50.17953 ↗
51. 10.1103/PhysRevLett.100.13640610.1103/PhysRevLett.100.136406 ↗
52. 10.1016/j.optmat.2024.11569310.1016/j.optmat.2024.115693 ↗
53. 10.1016/j.mser.2010.12.00110.1016/j.mser.2010.12.001 ↗
54. 10.1021/nl401066e10.1021/nl401066e ↗
55. 10.1063/1.274972810.1063/1.2749728 ↗
56. 10.1038/s41699-021-00226-z10.1038/s41699-021-00226-z ↗