Quantifying Temperature Dependence of Electronic Band Gaps and Optical Properties in SnO2 and SnO via First-Principles Simulations
Source abstract
Abstract
Tin metal oxides SnO x ( x = 1, 2) have gained interest as gas-sensing materials. For their applications as high-temperature sensors, however, a better understanding of their temperature dependence sensing responses is needed. In this work, we comparatively quantify the temperature-dependent electronic band gaps and optical properties of SnO 2 and SnO using first-principles calculations. Without considering the temperature effect, SnO 2 and SnO are predicted to have direct and indirect band gaps of 2.18 and 1.66 eV, respectively, at the PBE + U -GGA level that we employed. The temperature effect on the electronic and optical properties is captured by taking account of the electron–phonon interaction. Band gap renormalization with temperature is calculated via the Allen–Heine–Cardona theory. For both oxides, we find a monotonic decrease in the electronic band gap such that renormalization at zero point (0 K) is ∼−0.17 and ∼−0.52 eV at 1000 K. These results are also analyzed by employing an analytical equation that helps characterize the band gap shift with temperature. In addition, the optical properties at finite temperatures are simulated using the frozen-phonon method that combines electron–phonon coupling with the momentum matrix. As temperature increases, the optical property spectra are smoothed because of the smearing effect, which diminishes optical constants at shorter wavelengths. Our results are of interest for high-temperature functional materials in applications of optical detection.
Source: openalex_inverted_index · Quality: baseline
Research context
OpenAlex topics: Gas Sensing Nanomaterials and Sensors · ZnO doping and properties · Transition Metal Oxide Nanomaterials
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
National Energy Technology Laboratory, United States Department of Energy, Pittsburgh, Pennsylvania 15236, United States
Department of Mechanical Engineering and Materials Science, University of Pittsburgh, Pittsburgh, Pennsylvania 15261, United States
Funding
U.S. Department of Energy · National Energy Technology Laboratory
References (62)
Show source-provided references
1. Romanosky, R. R.; Maley, S. M. Harsh Environment Sensor Development for Advanced Energy Systems, Micro- and Nanotechnology Sensors, Systems, and Applications V; International Society for Optics and Photonics, 2013; p. 87250H.10.1117/12.2015865 ↗
2. 10.1063/1.369538010.1063/1.3695380 ↗
3. 10.1016/j.snb.2014.04.10610.1016/j.snb.2014.04.106 ↗
4. 10.1016/j.snb.2015.07.04610.1016/j.snb.2015.07.046 ↗
5. 10.1021/acsami.8b1195610.1021/acsami.8b11956 ↗
6. 10.1039/D0NR03306E10.1039/D0NR03306E ↗
7. 10.1039/b300617d10.1039/b300617d ↗
8. 10.1088/2040-8986/aa741910.1088/2040-8986/aa7419 ↗
9. Korotcenkov G. · 201410.1007/978-1-4614-7388-6 ↗
10. 10.1016/j.mseb.2007.01.04410.1016/j.mseb.2007.01.044 ↗
11. 10.1103/PhysRevMaterials.3.04460210.1103/PhysRevMaterials.3.044602 ↗
12. 10.1039/D0CP05445C10.1039/D0CP05445C ↗
13. 10.1039/C5NR00202H10.1039/C5NR00202H ↗
14. 10.1016/j.nanoen.2015.10.02610.1016/j.nanoen.2015.10.026 ↗
15. 10.1016/j.apcata.2019.11713410.1016/j.apcata.2019.117134 ↗
16. 10.1016/j.pmatsci.2014.06.00310.1016/j.pmatsci.2014.06.003 ↗
17. Aswal D. K. · 2006
18. 10.1103/PhysRevB.77.04533210.1103/PhysRevB.77.045332 ↗
19. 10.1142/S021797921650228310.1142/S0217979216502283 ↗
20. 10.1016/j.commatsci.2009.11.03810.1016/j.commatsci.2009.11.038 ↗
21. 10.1103/PhysRevLett.101.05550210.1103/PhysRevLett.101.055502 ↗
22. 10.1142/S021963361450069210.1142/S0219633614500692 ↗
23. 10.1021/jp205148y10.1021/jp205148y ↗
24. 10.1103/RevModPhys.77.117310.1103/RevModPhys.77.1173 ↗
25. 10.1063/1.492708110.1063/1.4927081 ↗
26. 10.1103/PhysRevB.92.08513710.1103/PhysRevB.92.085137 ↗
27. 10.1103/RevModPhys.89.01500310.1103/RevModPhys.89.015003 ↗
28. 10.1038/s41524-020-00434-z10.1038/s41524-020-00434-z ↗
29. 10.1021/acs.jpcc.8b0694110.1021/acs.jpcc.8b06941 ↗
30. 10.1088/1361-648X/ab9d4f10.1088/1361-648X/ab9d4f ↗
31. 10.1021/acs.jpclett.0c0018310.1021/acs.jpclett.0c00183 ↗
32. 10.1021/acsami.1c0350310.1021/acsami.1c03503 ↗
33. 10.1088/0022-3719/9/12/01310.1088/0022-3719/9/12/013 ↗
34. 10.1103/PhysRevB.23.149510.1103/PhysRevB.23.1495 ↗
35. 10.1063/1.10472310.1063/1.104723 ↗
36. 10.1088/0268-1242/31/11/11501610.1088/0268-1242/31/11/115016 ↗
37. 10.1103/PhysRevB.47.55810.1103/PhysRevB.47.558 ↗
38. 10.1016/0927-0256(96)00008-010.1016/0927-0256(96)00008-0 ↗
39. 10.1103/PhysRevB.50.1795310.1103/PhysRevB.50.17953 ↗
40. 10.1103/PhysRevLett.77.386510.1103/PhysRevLett.77.3865 ↗
41. 10.1088/0953-8984/9/4/00210.1088/0953-8984/9/4/002 ↗
42. 10.1063/1.338234410.1063/1.3382344 ↗
43. 10.1103/PhysRevB.13.518810.1103/PhysRevB.13.5188 ↗
44. 10.1103/PhysRevB.73.04511210.1103/PhysRevB.73.045112 ↗
45. 10.1016/j.jssc.2017.09.01610.1016/j.jssc.2017.09.016 ↗
46. 10.1016/j.scriptamat.2015.07.02110.1016/j.scriptamat.2015.07.021 ↗
47. 10.1103/RevModPhys.73.51510.1103/RevModPhys.73.515 ↗
48. 10.1016/S0927-0256(02)00325-710.1016/S0927-0256(02)00325-7 ↗
49. 10.1016/j.cpc.2016.04.00310.1016/j.cpc.2016.04.003 ↗
50. 10.1103/PhysRevB.88.08511710.1103/PhysRevB.88.085117 ↗
51. 10.1016/j.vacuum.2020.10942810.1016/j.vacuum.2020.109428 ↗
52. 10.1063/1.353210910.1063/1.3532109 ↗
53. 10.1016/j.optmat.2014.10.01710.1016/j.optmat.2014.10.017 ↗
54. Patnaik P. · 2003
55. 10.1021/acs.jpclett.6b0256010.1021/acs.jpclett.6b02560 ↗
56. 10.1021/acs.jpclett.8b0316410.1021/acs.jpclett.8b03164 ↗
57. 10.1149/1.213264710.1149/1.2132647 ↗
58. 10.1103/PhysRev.78.808.210.1103/PhysRev.78.808.2 ↗
59. 10.1016/S0065-2539(08)60957-910.1016/S0065-2539(08)60957-9 ↗
60. 10.1103/PhysRevLett.48.40610.1103/PhysRevLett.48.406 ↗
61. 10.1103/PhysRevB.92.18430110.1103/PhysRevB.92.184301 ↗
62. 10.1103/PhysRevB.94.07512510.1103/PhysRevB.94.075125 ↗