DOI:
10.1039/D4RA05885B
(Comment)
RSC Adv., 2024,
14, 33794-33796
Reply to the ‘Comment on “Improving the efficiency of a CIGS solar cell to above 31% with Sb2S3 as a new BSF: a numerical simulation approach by SCAPS-1D”’ by A. Kirk, RSC Adv., 2024, https://doi.org/10.1039/D4RA03002H
Received
13th August 2024
, Accepted 27th September 2024
First published on 24th October 2024
Our Reply for Alexander P. Kirk comment
We sincerely appreciate the thoughtful feedback on our manuscript (https://doi.org/10.1039/D3RA07893K). In the comment, Alexander P. Kirk has referenced a reported efficiency of 40.70% for our solar cell design. However, we would like to clarify that the actual efficiency of our CIGS solar cell (Copper Indium Gallium Selenide) with the addition of a new BSF (back surface field) layer made from Sb2S3 (Antimony Sulfide) is 31.15%. When the BSF layer is not used, the efficiency is 22.14%.1 To ensure transparency and accuracy, these efficiency values have been clearly stated at multiple points throughout our manuscript. Specifically, the efficiency data is provided in the following sections: (i) Title, (ii) Abstract, (iii) Introduction, (iv) Results and discussion, (v) J–V parts, Table 1, and Table 2, and (vi) Conclusions in the reputed manuscript.1 By mentioning the efficiency values in multiple sections, we have taken steps to avoid any confusion and ensure clarity regarding the performance of our solar cell both with and without the BSF layer. In Fig. 1, we have shown the proposed CIGS solar cell with Sb2S3 BSF layer.
Table 1 PV performance of suggested cell compared to other reported CIGS solar cell without BSF
Types of research |
CIGS layer thickness (μm) |
VOC (V) |
JSC (mA cm−2) |
FF (%) |
η (%) |
Ref. |
Experimental |
2.0 |
0.671 |
34.90 |
77.60 |
18.10 |
2 |
Experimental |
1.0 |
0.689 |
35.71 |
78.12 |
19.20 |
3 |
Experimental |
2.2 |
0.690 |
35.50 |
81.20 |
19.90 |
4 |
Experimental |
— |
0.741 |
37.80 |
80.60 |
22.60 |
5 |
Theoretical |
1.0 |
0.743 |
34.47 |
83.09 |
21.30 |
6 |
Theoretical |
1.0 |
0.91 |
28.21 |
86.31 |
22.14* (without BSF) |
*This work |
Table 2 Impact of BSF layer in comparison with related research
Types of research |
Absorber |
BSF |
η without BSF (%) |
η with BSF (%) |
Ref. |
Experimental |
Si |
ZnS |
6.40 |
11.02 |
7 |
Experimental |
Si |
Al |
12.96 |
13.75 |
8 |
Experimental |
CIGS |
MoSe2 |
9 |
14 |
9 |
Theoretical |
CdTe |
V2O5 |
19.58 |
23.50 |
10 |
Theoretical |
CZTS |
CZTS |
12.05 |
14.11 |
11 |
Theoretical |
ZnTe |
Sb2Te3 |
7.14 |
18.33 |
12 |
Theoretical |
CZTSSe |
SnS |
12.30 |
17.25 |
13 |
Theoretical |
CIGS |
Si |
16.39 |
21.30 |
6 |
Theoretical |
CIGS |
μc-Si:H |
19.80 |
23.42 |
14 |
Theoretical |
CIGS |
SnS |
17.99 |
25.29 |
15 |
Theoretical |
CIGS |
PbS |
22.67 |
24.22 |
16 |
Theoretical |
CIGS |
Sb2S3 |
22.14* |
31.15* |
*This work |
|
| Fig. 1 Proposed CIGS solar cell with Sb2S3 BSF layer. | |
In contrast to the comment, I have utilized all the optimized parameters listed in Tables 3 and 4 for our proposed solar cell structure (FTO/SnS2/CIGS/Sb2S3/Ni) in the SCAPS-1D simulation. To determine the optimal absorber thickness, we conducted an extensive analysis, varying the thickness from 250 nm to 3000 nm. Across this range, the power conversion efficiency of our proposed structure varied from 19.80% to a maximum of 40.70%. It is important to note that the 40.70% efficiency does not represent the optimized efficiency for the solar cell. After a thorough investigation, we identified that an absorber thickness of 1 μm (1000 nm) is optimal. This specific thickness, as shown in Tables 3 and 4,1 provided efficiencies of 31.15% when using the Sb2S3 BSF layer and 22.14% without it. Therefore, the optimized efficiency with the 1 μm absorber is significantly lower than the 40.70% figure mentioned, which is the highest efficiency obtained during the range of testing but not the optimal one.
Table 3 Layer properties used in Al/FTO/SnS2/CIGS/Sb2S3/Ni solar cella17–20
Parameters (unit) |
FTO |
SnS2 |
CIGS |
Sb2S3 |
SA single acceptor, SD single donor, (*) variable field. |
Layer type |
Window |
ETL |
Absorber |
BSF |
Conductivity type |
n+ |
n |
p |
P+ |
Thickness (μm) |
0.05 |
0.05 |
1.0* |
0.2 |
Bandgap (eV) |
3.6 |
2.24 |
1.1 |
1.62 |
Electron affinity (eV) |
4 |
4.24 |
4.2 |
3.70 |
Dielectric permittivity (relative) |
9 |
10 |
13.6 |
7.08 |
CB effective DOS (cm−3) |
2.2 × 1018 |
2.2 × 1018 |
2.2 × 1018 |
2.0 × 1019 |
VB effective DOS (cm−3) |
1.8 × 1019 |
1.8 × 1019 |
1.8 × 1019 |
1.0 × 1019 |
Electron thermal velocity (cm s−1) |
1 × 107 |
1 × 107 |
1 × 107 |
1 × 107 |
Hole thermal velocity (cm s−1) |
1 × 107 |
1 × 107 |
1 × 107 |
1 × 107 |
Electron mobility (cm2 V−1 s−1) |
100 |
50 |
100 |
9.8 |
Hole mobility (cm2 V−1 s−1) |
25 |
50 |
25 |
10 |
Donor density, ND (cm−3) |
1 × 1018 |
1 × 1015 |
0 |
0 |
Acceptor density, NA (cm−3) |
0 |
0 |
1 × 1016* |
1 × 1015 |
Defect type |
SA |
SA |
SD |
SD |
Defect density (cm−3) |
1 × 1012 |
1 × 1012 |
1 × 1012 |
1 × 1012 |
Table 4 Interface factors used in Al/FTO/SnS2/CIGS/Sb2S3/Ni solar cell
Parameters (unit) |
Sb2S3/CIGS interface |
CIGS/SnS2 interface |
Defect type |
Neutral |
Neutral |
Electron capture cross-section, σe (cm2) |
1 × 1019 |
1 × 1019 |
Hole capture cross-section, σp (cm2) |
1 × 1019 |
1 × 1019 |
Defect position above the highest EV (eV) |
0.06 |
0.06 |
Interface defect density (cm−2) |
1 × 1012 |
1 × 1012 |
Additionally, Alexander P. Kirk raised concerns regarding our consideration of hot carrier collection in the manuscript. However, it is crucial to highlight that in Tables 3 and 4, we have presented all the optimized parameters used in our SCAPS-1D simulation, which includes all relevant factors for accurately simulating the performance of our solar cell structure. The results are reflective of the carefully optimized conditions, and hot carrier collection was not an assumed factor in our analysis. By clarifying the distinction between the highest and optimized efficiencies and addressing the concerns about parameter usage, we ensure that the results and methods presented are accurate and consistent with the scope of the study.
Ethical approval
The all authors declare that the manuscript does not have studies on human subjects, human data or tissue, or animals.
Data availability
Data will be available on request.
Conflicts of interest
The authors have no conflicts of interest.
Acknowledgements
A. Irfan extends his appreciation to the Deanship of Research and Graduate Studies at King Khalid University for funding this work through Large Groups Research Project under grant number RGP.2/146/45. A. R. Chaudhry is thankful to the Deanship of Graduate Studies and Scientific Research at the University of Bisha for supporting this work through the Fast-Track Research Support Program.
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