Acoustic shock wave-induced B1 to B2 phase transition of CdO nanoparticles: Structure-property relationship and its mechanism in thermodynamic aspects
Source abstract
Abstract
The reversible pressure-induced B1 (NaCl) ↔ B2 (CsCl)-type phase transition is one of the classic models for understanding the general concepts of phase transition. Although several outstanding functional properties have been identified for B2 phase materials under high-pressure conditions, generating a stable B2 phase under ambient conditions is a critical task for device fabrication. Herein, we report a novel B1-B2-type phase transition in cadmium oxide nanoparticles (CdO NPs) by millisecond-low-pressure acoustic shock waves (16.5 MPa and 3173 K) that is highly stable under ambient conditions. Under static high-pressure conditions, the B1-B2 phase transition requires ∼102 GPa, which is reversible. A new thermodynamic mechanism is proposed to explain the B1-B2 transition considering the thermal conductivity, whereby materials with low thermal conductivity undergo significant structural phase transitions under acoustic shocked conditions. Herein, we consider several nanosized materials for structural stability, including B1 (CdO, MgO, NiO), Corundum (α-Fe 2O 3, α-Al 2O 3), layered (graphene, graphite) and nonlayered (TiO 2 (anatase), ZnO (B4) and amorphous carbon) materials, under acoustic shocked conditions, which fall within the proposed mechanism.
Source: expertdata · Quality: candidate unverified · Source record ↗
Research context
OpenAlex topics: Laser-Ablation Synthesis of Nanoparticles · Quantum Dots Synthesis And Properties · Boron and Carbon Nanomaterials Research
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
References (63)
Show source-provided references
1. Melting of LiF and NaCl to 1 Mbar: systematics of ionic solids at extreme conditions10.1103/PhysRevLett.78.4589 ↗
2. Experimental evidence for a phase transition in magnesium oxide at exoplanet pressures10.1038/ngeo1948 ↗
3. Equation of state of MgO up to 345 GPa and 8500 K
4. Toward an accurate equation of state and B1-B2 phase boundary for magnesium oxide up to terapascal pressures and electron-volt temperatures10.1103/PhysRevB.107.224109 ↗
5. Pressure-volume equation of state of the high-pressure B2 phase of NaCl10.1103/PhysRevB.65.104114 ↗
6. Ab initio calculations of the B1-B2 phase transition in MgO10.1103/PhysRevB.99.094113 ↗
7. Ultrafast X-ray diffraction visualization of B1-B2 phase transition in KCl under shock compression
8. Transformation of shock-compressed graphite to hexagonal diamond in nanoseconds10.1126/sciadv.aao3561 ↗
9. Acoustic shock wave-induced solid-state fusion of nanoparticles: a case study of the conversion of one-dimensional rod shape into three-dimensional honeycomb nanostructures of CdO for high performance energy storage materials10.1021/acs.inorgchem.3c03461 ↗
10. Measurement of the B1-B2 transition pressure in NaC1 at high temperatures10.1103/PhysRevB.36.474 ↗
11. Time-resolved infrared radiometry of NaCl crystals under shock compression between 17 and 43 GPa10.1103/PhysRevB.70.144110 ↗
12. Femtosecond diffraction studies of the sodium chloride phase diagram under laser shock compression10.1063/5.0094894 ↗
13. Direct conversion of graphite to diamond in static pressure apparatus10.1126/science.137.3535.1057 ↗
14. Role of graphite crystal structure on the shock-induced formation of cubic and hexagonal diamond10.1103/PhysRevB.101.224109 ↗
15. Nanosecond formation of diamond and lonsdaleite by shock compression of graphite10.1038/ncomms10970 ↗
16. Acoustic shock wave-induced sp2-to-sp3-type phase transition: a case study of a graphite single crystal10.1039/D4TC03216K ↗
17. Acoustic shock wave induced chemical reactions - A case study of NaCl single crystal
18. Dynamic shock wave driven simultaneous crystallographic and molecular switching between α-Fe2O3 and Fe3O4 nanoparticles–a new finding10.1039/D2DT01101H ↗
19. Dynamic shock wave-induced amorphous-to-crystalline switchable phase transition of lithium sulphate10.1021/acs.jpcc.1c09411 ↗
20. High-pressure structural studies of hematite Fe2O3. Phys
21. High-pressure phase transitions in Li2SO410.1103/PhysRevB.41.11593 ↗
22. A. Amouretti, C. Crépisson, S. Azadi, D. Cabaret, T. Campbell, D.A. Chin, B. Colin, G.R. Collins, L. Crandall, G. Fiquet, A. Forte, T. Gawne, F. Guyot, P. Heighway, H. Lee, D. McGonegle, B. Nagler, J. Pintor, D. Polsin, G. Rousse, Y. Shi, E. Smith, J.S. Wark, S.M. Vinko, M. Harmand, Phase transitions of Fe2O3 under laser shock compression. (2024). DOI: https://doi.org/10.48550/arXiv.2402.18432.
23. B1-to-B2 phase transition of transition-metal monoxide CdO under strong compression10.1103/PhysRevB.70.094114 ↗
24. First principles calculations of the ground-state properties and structural phase transformation in CdO
25. Ab initio determination of X-ray structure factors and the Compton profiles of CdO10.1016/j.jallcom.2010.04.060 ↗
26. Manually operated piston-driven shock tube
27. Shock tube design for high intensity blast waves for laboratory testing of armor and combat materiel10.1016/j.dt.2014.04.003 ↗
28. Measurement of “shock wave parameters” in a novel table-top shock tube using microphones10.1007/s41314-019-0033-5 ↗
29. Investigation of CdO hexagonal nanoflakes synthesized by hydrothermal method for liquefied petroleum gas detection10.1039/C6AY01914E ↗
30. Temperature-dependent optical properties of epitaxial CdO thin films determined by spectroscopic ellipsometry and Raman scattering10.1063/1.4803876 ↗
31. Investigation of chemical bath deposition of CdO thin films using three different complexing agents10.1016/j.apsusc.2011.04.060 ↗
32. Exploration of CdO properties favouring superior photocatalytic degradation of methylene blue dye by Al3+ doping10.1007/s11082-022-03694-9 ↗
33. Optimization of CdO nanoparticles by Zr4+ doping for better photocatalytic activity
34. First-principles study of ground- and excited-state properties of MgO, ZnO, and CdO polymorphs10.1103/PhysRevB.73.245212 ↗
35. Valence-band electronic structure of CdO, ZnO, and MgO from X-ray photoemission spectroscopy and quasiparticle-corrected density-functional theory calculations10.1103/PhysRevB.79.205205 ↗
36. Experimental demonstration of acoustic shockwave-induced solid-state morphological transformation from irregular to rod shape: a case study of L-tyrosine10.1039/D3CE01002C ↗
37. Experimental evidence of acoustic shock wave-induced dynamic recrystallization: a case study on ammonium sulfate10.1021/acs.cgd.3c01180 ↗
38. Collective magnetic response of CeO2 nanoparticles10.1038/nphys3676 ↗
39. Ferromagnetism as a universal feature of nanoparticles of the otherwise nonmagnetic oxides10.1103/PhysRevB.74.161306 ↗
40. Comparative investigation of physicochemical properties of cadmium oxide nanoparticles10.1016/j.ceramint.2021.10.204 ↗
41. Relation between thermal expansivity and bulk modulus for ionic solids at high temperatures10.1016/j.physb.2003.12.020 ↗
42. Facile synthesis of CdO nanorods and exploiting its properties towards supercapacitor electrode materials and low power UV irradiation driven photocatalysis against methylene blue dye10.1016/j.materresbull.2017.02.044 ↗
43. Honeycomb-based heterostructures: An emerging platform for advanced energy applications: A review on energy systems10.1002/elsa.202100075 ↗
44. Shock waves induced enhancement of electrochemical properties of CoFe2O4 nanoparticles for energy storage applications
45. Pseudocapacitive oxide materials for high-rate electrochemical energy storage10.1039/c3ee44164d ↗
46. Where do batteries end and supercapacitors begin?10.1126/science.1249625 ↗
47. Vacancies in MgO at ultrahigh pressure: about mantle rheology of super-Earths10.1016/j.icarus.2017.12.020 ↗
48. Phase transformations and metallization of magnesium oxide at high pressure and temperature10.1126/science.1229450 ↗
49. Synthesis of crystalline graphite from disordered graphite by acoustic shock waves: hot-spot nucleation approach
50. Acoustic shock wave-induced ordered to disordered switchable phase transitions: a case study of ferroelectric triglycine sulphate single crystal for the application of molecular switches
51. Acoustic shock wave-induced rutile to anatase phase transition of TiO2 nanoparticles and exploration of their unconventional thermodynamic structural transition path of crystallization behaviors10.1021/acs.inorgchem.4c02723 ↗
52. Nanosecond melting and recrystallization in shock-compressed silicon10.1103/PhysRevLett.121.135701 ↗
53. Shock-induced superheating and melting curves of geophysically important minerals10.1016/j.pepi.2003.04.001 ↗
54. Shock–induced melting and shear banding in single–crystal NaCl10.1063/1.340469 ↗
55. Melting of Cu under hydrostatic and shock wave loading to high pressures
56. Thermal conductivity and secondary porosity of single anatase TiO2 nanowire10.1088/0957-4484/23/18/185701 ↗
57. Thermal conductivity of amorphous carbon thin films10.1063/1.1314301 ↗
58. Thermal conductivity of graphene and graphite10.1103/PhysRevB.87.115421 ↗
59. Calculated transport properties of CdO: thermal conductivity and thermoelectric power factor10.1103/PhysRevB.92.144301 ↗
60. Thermal conductivity calculation in anisotropic crystals by molecular dynamics: application to α-Fe2O310.1063/1.4974933 ↗
61. Thermal diffusivity and thermal conductivity of single–crystal MgO and Al2O3 and related compounds as a function of temperature10.1007/s00269-014-0655-3 ↗
62. Microstructure and thermal conductivity of surfactant-free NiO nanostructures10.1016/j.jssc.2012.01.052 ↗
63. Thermal conductivity of II-VI compounds and phonon scattering by Fe2+ impurities10.1103/PhysRevB.6.3791 ↗