journal article·2026-03-01Open access

Influence of carbon atoms in single crystal Si on electron trap generation due to UV light irradiation during RPD process

Subhash Chand Yadav, Keita Kimura, Tomohiko Hara, Yoshio Ohshita

AIP Advances· Volume 16· Issue 3

Abstract

The recombination-active defects in crystalline silicon are generated during the solar cell fabrication by the ultraviolet light in the reactive plasma deposition (RPD) process, which degrades carrier lifetime and limits the performance of high-efficiency solar cells. Although previous studies have linked these defects to oxygen-related complexes, the possible influence of carbon impurities remains unclear. In this study, the correlation between the bulk carbon (C) concentration and the RPD-induced defect formation in Czochralski-grown single-crystal silicon was systematically investigated using deep-level transient spectroscopy (DLTS). Silicon wafers with C concentrations ranging from 1.3 × 1014 to 6.0 × 1016 cm−3 and with nearly constant oxygen content (∼1.8 × 1018–2.0 × 1018 cm−3) were processed under identical RPD conditions. DLTS revealed three distinct electron traps (E1, E2, and E3) located within ∼200 nm from the SiO2/Si interface. Their energy levels, capture cross sections, and concentrations were nearly invariant across the C range. The results indicated that the recombination centers created by the RPD process are very likely related to oxygen-related species, i.e., O–Si divacancies, based on the parameter values determined. This work refines the understanding of plasma-induced defect mechanisms and supports optimized RPD processing for reliable, high-efficiency carrier-selective contact (CSC) solar cells.
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Research context

OpenAlex topics: Silicon and Solar Cell Technologies · Thin-Film Transistor Technologies · solar cell performance optimization

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

Affiliations

Semiconductor Laboratory, Toyota Technological Institute 1 , Nagoya, 468-8511 Aichi,

Ritsumeikan University 2 , Kusatsu, 525-8577 Shiga,

References (32)

Show source-provided references
1. 23.5%-efficient silicon heterojunction silicon solar cell using molybdenum oxide as hole-selective contact10.1016/j.nanoen.2020.104495 ↗
2. High-efficiency silicon heterojunction solar cells: Materials, devices and applications10.1016/j.mser.2020.100579 ↗
3. Conductive and stable magnesium oxide electron-selective contacts for efficient silicon solar cells10.1002/aenm.201601863 ↗
4. Influence of ITO deposition and post annealing on HIT solar cell structures10.1016/j.egypro.2011.06.125 ↗
5. Precipitation of oxygen and intrinsic gettering in silicon10.1557/proc-2-367 ↗
6. DLTS analysis of interface and near-interface bulk defects induced by TCO-plasma deposition in carrier-selective contact solar cells10.1063/5.0177685 ↗
7. Oxygen precipitation behavior in n-type Cz-Si related to carbon concentration and crystal growth conditions10.1007/s11664-020-08702-w ↗
8. Generation of oxygen-related defects in crystal silicon processed by the RPD10.3390/cryst13020310 ↗
9. Carbon-isovalent dopant pairs in silicon: A density functional theory study10.3390/app14104194 ↗
10. Analysis of damage created by ion implantation in GaAs using process simulation10.1063/1.349245 ↗
11. Investigation of ppb-level surface contamination of n-type silicon solar cells10.1016/j.apsusc.2020.146299 ↗
12. Powerful recombination centers resulting from reactions of hydrogen with carbon–oxygen defects in n-type Czochralski-grown silicon10.1002/pssr.201700133 ↗
13. Properties of defects and charge centers in the SiO2/Si of CSC solar cells induced by reactive plasma deposition
14. Light induced recombination center at SiO2/Si interface by the reactive plasma deposition10.1007/s13391-021-00295-8 ↗
15. Performance analysis of silicon carrier selective contact solar cells with ALD MoOx as hole selective layer10.1007/s12633-021-00984-x ↗
16. Silicon heterojunction solar cell with interdigitated back contacts for a photoconversion efficiency over 26%10.1038/nenergy.2017.32 ↗
17. Room-temperature sputtered tungsten-doped indium oxide for improved current in silicon heterojunction solar cells10.1016/j.solmat.2021.111082 ↗
18. Effects of damages induced by indium-tin-oxide reactive plasma deposition on minority carrier lifetime in silicon crystal10.1063/1.5124903 ↗
19. A study of deep levels in GaAs by capacitance spectroscopy10.1007/BF02660189 ↗
20. Deep level transient Fourier spectroscopy (DLTFS)—A technique for the analysis of deep level properties10.1016/0038-1101(88)90071-8 ↗
21. DLTFS investigation of InGaAsN/GaAs tandem solar cell10.2478/jee-2014-0043 ↗
22. Silicon heterojunction solar cells with electron selective TiOx contact10.1016/j.solmat.2016.01.020 ↗
23. Deep-level transient spectroscopy: A new method to characterize traps in semiconductors10.1063/1.1663719 ↗
24. Silicon heterojunction solar cells: Recent technological development and practical aspects - From lab to industry10.1016/j.solmat.2018.07.018 ↗
25. Towards bifacial silicon heterojunction solar cells with reduced TCO use10.1002/pip.3550 ↗
26. Effect of front TCO on the performance of rear-junction silicon heterojunction solar cells: Insights from simulations and experiments10.1016/j.solmat.2019.01.047 ↗
27. DLTS DLTS with Bayesian inference for analyzing RPD induced defects in bulk near SiO2/Si interface10.1149/2162-8777/ac5806 ↗
28. Deep-level-transient spectroscopy: System effects and data analysis10.1063/1.326665 ↗
29. Evaluation of damage in crystalline silicon substrate induced by plasma enhanced chemical vapor deposition of amorphous silicons film10.1149/2162-8777/acb4bb ↗
30. Development of new a-Si/c-Si heterojunction solar cells: ACJ-HIT (artificially constructed junction-heterojunction with intrinsic thin-layer)10.1143/JJAP.31.3518 ↗
31. Evaluation of plasma induced defects on silicon substrate by solar cell fabrication process10.35848/1347-4065/ab984d ↗
32. Analysis of recombination centers near an interface of a metal–SiO2–Si structure by double carrier pulse deep-level transient spectroscopy10.1063/5.0106319 ↗