Optically Determined Hole Effective Mass in Tin-Iodide Perovskite Films
Source abstract
Abstract
High Resolution Image Download MS PowerPoint Slide Tin-halide perovskites currently offer the best photovoltaic performance of lead-free metal-halide semiconductors. However, their transport properties are mostly dominated by holes, owing to ubiquitous self-doping. Here we demonstrate a noncontact, optical spectroscopic method to determine the effective mass of the dominant hole species in FASnI 3, by investigating a series of thin films with hole densities finely tuned through either SnF 2 additive concentration or controlled exposure to air. We accurately determine the plasma frequency from mid-infrared reflectance spectra by modeling changes in the vibrational response of the FA cation as the plasma edge shifts through the molecular resonance. Our approach yields a hole effective mass of 0.28 m e for FASnI 3 and demonstrates parabolicity within ∼100 meV of the valence band edge. An absence of Fano contributions further highlights insignificant coupling between the hole plasma and FA cation. Overall, this approach enables noncontact screening of thin-film materials for optimized charge-carrier transport properties.
Source: openalex_inverted_index · Quality: baseline
Research context
OpenAlex topics: Perovskite Materials and Applications · Electronic and Structural Properties of Oxides · Magnetic and transport properties of perovskites and related materials
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Department of Physics, Clarendon Laboratory, University of Oxford, Parks Road, Oxford OX1 3PU, U.K.
School of Physics and Astronomy
University of Birmingham
Funding
Engineering and Physical Sciences Research Council
References (63)
Show source-provided references
1. 10.1021/acsenergylett.1c0063610.1021/acsenergylett.1c00636 ↗
2. 10.1021/acsaem.3c0232710.1021/acsaem.3c02327 ↗
3. 10.1021/acsmaterialslett.2c0082910.1021/acsmaterialslett.2c00829 ↗
4. 10.1021/acs.chemmater.3c0318610.1021/acs.chemmater.3c03186 ↗
5. 10.1021/acsenergylett.3c0140010.1021/acsenergylett.3c01400 ↗
6. 10.1039/C6MH00519E10.1039/C6MH00519E ↗
7. 10.1002/adma.20180379210.1002/adma.201803792 ↗
8. 10.1002/smtd.20230020710.1002/smtd.202300207 ↗
9. 10.1002/adma.20190739210.1002/adma.201907392 ↗
10. 10.1002/smll.20250187610.1002/smll.202501876 ↗
11. 10.1038/s41586-018-0691-010.1038/s41586-018-0691-0 ↗
12. 10.1039/D3NA00319A10.1039/D3NA00319A ↗
13. 10.1002/adma.20210584410.1002/adma.202105844 ↗
14. 10.1021/acsenergylett.4c0317210.1021/acsenergylett.4c03172 ↗
15. 10.1006/jssc.1995.102310.1006/jssc.1995.1023 ↗
16. 10.1016/j.jssc.2013.07.00810.1016/j.jssc.2013.07.008 ↗
17. 10.1021/ja301539s10.1021/ja301539s ↗
18. 10.1021/ic401215x10.1021/ic401215x ↗
19. 10.1002/aenm.20230291610.1002/aenm.202302916 ↗
20. 10.1002/adma.20180450610.1002/adma.201804506 ↗
21. 10.1039/C4EE01076K10.1039/C4EE01076K ↗
22. 10.1038/srep0446710.1038/srep04467 ↗
23. 10.1002/adfm.20230789610.1002/adfm.202307896 ↗
24. 10.1039/D5CS00340G10.1039/D5CS00340G ↗
25. 10.1002/pssr.20130818310.1002/pssr.201308183 ↗
26. 10.1021/acs.jpclett.0c0072510.1021/acs.jpclett.0c00725 ↗
27. 10.1021/acsenergylett.7b0063610.1021/acsenergylett.7b00636 ↗
28. 10.1002/aenm.20220084710.1002/aenm.202200847 ↗
29. 10.1021/acsenergylett.1c0077610.1021/acsenergylett.1c00776 ↗
30. 10.1021/acsenergylett.0c0179610.1021/acsenergylett.0c01796 ↗
31. 10.1002/advs.20190354010.1002/advs.201903540 ↗
32. 10.1002/adfm.20200559410.1002/adfm.202005594 ↗
33. 10.1039/D2MH00008C10.1039/D2MH00008C ↗
34. 10.1039/C5EE03435C10.1039/C5EE03435C ↗
35. 10.1021/acsenergylett.8b0224310.1021/acsenergylett.8b02243 ↗
36. 10.1021/acsenergylett.0c0116610.1021/acsenergylett.0c01166 ↗
37. 10.1016/j.commatsci.2019.10911810.1016/j.commatsci.2019.109118 ↗
38. 10.1021/acs.jpcc.7b1197610.1021/acs.jpcc.7b11976 ↗
39. 10.1021/acs.jpcc.8b0401310.1021/acs.jpcc.8b04013 ↗
40. 10.1039/D0RA02584D10.1039/D0RA02584D ↗
41. 10.1021/jp506498k10.1021/jp506498k ↗
42. 10.1002/solr.20210006910.1002/solr.202100069 ↗
43. 10.1039/C5TA00190K10.1039/C5TA00190K ↗
44. 10.1002/adom.20170061510.1002/adom.201700615 ↗
45. 10.1021/acsenergylett.8b0234610.1021/acsenergylett.8b02346 ↗
46. 10.1021/acsenergylett.4c0255810.1021/acsenergylett.4c02558 ↗
47. Schubert E. F. · 199310.1017/CBO9780511599828 ↗
48. 10.1103/PhysRev.182.52610.1103/PhysRev.182.526 ↗
49. 10.1002/pssb.20135003910.1002/pssb.201350039 ↗
50. 10.1002/adom.20210155310.1002/adom.202101553 ↗
51. 10.1021/acs.jpclett.8b0281110.1021/acs.jpclett.8b02811 ↗
52. 10.1021/acs.jpcc.5b0743210.1021/acs.jpcc.5b07432 ↗
53. 10.1021/acs.jpclett.5b0130910.1021/acs.jpclett.5b01309 ↗
54. 10.1103/PhysRev.124.186610.1103/PhysRev.124.1866 ↗
55. 10.1038/nphoton.2017.14210.1038/nphoton.2017.142 ↗
56. 10.1088/1402-4896/abe58010.1088/1402-4896/abe580 ↗
57. 10.1002/anie.20180667610.1002/anie.201806676 ↗
58. 10.1038/s41467-022-31416-y10.1038/s41467-022-31416-y ↗
59. Fox A. M. · 2012
60. 10.1002/solr.20180013210.1002/solr.201800132 ↗
61. 10.1021/jz402386510.1021/jz4023865 ↗
62. 10.1038/srep2861810.1038/srep28618 ↗
63. 10.1002/adma.20140199110.1002/adma.201401991 ↗