2022
DOI: 10.1007/s10825-021-01843-z
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Numerical investigation of the effects of copper sulfide nanoparticles on hole transport layer of thin-film organic solar cells

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Cited by 7 publications
(7 citation statements)
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“…Even though P 3 HT: PC 61 BM-based OSCs are lightweight, have a large area of coverage, and are low-cost to fabricate, the potential commercialization of OSC has not yet been entirely accomplished [29]. One plausible issue is that the most common anode material used in OSC is a transparent conductive oxide (TCO), which is expensive to produce and has some undesirable features [30].…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…Even though P 3 HT: PC 61 BM-based OSCs are lightweight, have a large area of coverage, and are low-cost to fabricate, the potential commercialization of OSC has not yet been entirely accomplished [29]. One plausible issue is that the most common anode material used in OSC is a transparent conductive oxide (TCO), which is expensive to produce and has some undesirable features [30].…”
Section: Introductionmentioning
confidence: 99%
“…The input material parameters used in the P 3 HT: PC 61 BM OSC device is based on previously tested values for the various consecutive layers. Here the symbols used for parameters are thickness (W), bandgap (E g ), relative permittivity (ε r ), electron affinity (χ i ), electron mobility (μ n ), hole mobility (μ p ), effective DOS at CB (N C ), effective DOS at VB (N V ), electron trap density (N e exp ), hole trap density (N h exp ), electron tail slope (N n U ), hole tail slope (N h U ), respectively[8][9][10][11][22][23][24][25][26][27][28][29][30][31][32][33][34][35][36][37]. Performance of OAL thickness with variable TCO in OSC After the optimization of TCO's thickness, the maximum value of device parameters would be achieved through the optimum thickness of OAL.…”
mentioning
confidence: 99%
“…Hence, in order to get more information about our fabricated solar cells, we performed numerical simulations using solar cells capacitance software (version 3.3.07). The program is a one-dimensional solar device simulator that was developed by Prof. Burgelman at the University of Gent, Belgium. , The simulation was based on the effective medium model, , in which the active layer (composed of the donor and acceptor materials) is described by a single semiconducting layer. Selective contacts or buffer layers are introduced to provide the migration driving force for the photo-generated electron–hole pairs generated. , The material properties for the effective medium are obtained from either PTB7-Th, ITIC-Th, or an average of both and are summarized in Table .…”
Section: Resultsmentioning
confidence: 99%
“…The program is a one-dimensional solar device simulator that was developed by Prof. Burgelman at the University of Gent, Belgium. 47,48 The simulation was based on the effective medium model, 49,50 in which the active layer (composed of the donor and acceptor materials) is described by a single semiconducting layer. Selective contacts or buffer layers are introduced to provide the migration driving force for the photo-generated electron−hole pairs generated.…”
Section: Resultsmentioning
confidence: 99%
“…On the other hand, a limited range of optical absorptions, a thin layer of polymer solar absorber, and short exciton diffusion length in polymer medium determine the growth of PCE in PSC. Moreover, the low carrier mobilities of the conducting polymers and the short lifetime of the exciton restrict the active layer thickness below 200 nm, so it is not possible to boost optical absorption by merely increasing the thickness [8][9][10][11][12][13][14]. Thus, in addition to the absorber layer composition and device architecture, the PCE in TFPSCs depends on the augmentation of the open-circuit voltage and the fill factor (FF) [15][16][17].…”
Section: Introductionmentioning
confidence: 99%