2017
DOI: 10.1039/c7ta07014d
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Efficient PbS quantum dot solar cells employing a conventional structure

Abstract: New-generation solar cells based on colloidal lead chalcogenide (PbX) quantum dots (CQDs) are promising low-cost solution-processed photovoltaics.

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Cited by 112 publications
(70 citation statements)
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“…Furthermore, the reduced energy barrier between conduction band of TiO 2 (−4.0 eV) and that of perovskite (Figure S11, Supporting Information) as well as the valence band of perovskite and work function of carbon electrode facilitates the electron injection and hole extraction, and therefore eliminating the radiative recombination . As expected, bimolecular charge recombination behavior is reduced ( α ≈ 1, Figure b) for doped perovskite solar cells according to the following relation: J sc ∝ I α , where I represents the incident light intensity, α is a factor related to recombination.…”
Section: Resultsmentioning
confidence: 71%
“…Furthermore, the reduced energy barrier between conduction band of TiO 2 (−4.0 eV) and that of perovskite (Figure S11, Supporting Information) as well as the valence band of perovskite and work function of carbon electrode facilitates the electron injection and hole extraction, and therefore eliminating the radiative recombination . As expected, bimolecular charge recombination behavior is reduced ( α ≈ 1, Figure b) for doped perovskite solar cells according to the following relation: J sc ∝ I α , where I represents the incident light intensity, α is a factor related to recombination.…”
Section: Resultsmentioning
confidence: 71%
“…When irradiating solar cells under graded‐regulated incident light intensity, the evolution of J sc and V oc can be employed to estimate the charge transport processes. By plotting J sc and V oc as a function of incident light intensity ( I ), as shown in Figure c,d, the interior recombination mechanism can be understood according to the following equationsJscIα(α1)Voc=nkTeln(I)+constantwhere the k is the Boltzmann constant, T is absolute temperature, e refers to elementary charge, α and n are ideal factors related to recombination. The bimolecular radiative recombination is expected to be minimal when a device is in short‐circuit condition, that is, α = 1 and the power output is maximal.…”
Section: Resultsmentioning
confidence: 99%
“…This is in agreement with the J – V and EQE measurements in Figure . To further investigate the charge recombination kinetics in the reference and Co 3 O 4 ‐PSC, the J sc and V oc as a function of illumination intensity have been studied, as seen in Figure c and d. According to the power law equation: JscIα, where I is the light intensity and α is the exponential factor. As shown in Figure c, the values of α for Co 3 O 4 ‐PSC and reference PSC are 0.9896 and 0.9755, respectively.…”
Section: Resultsmentioning
confidence: 99%
“…As shown in Figure c, the values of α for Co 3 O 4 ‐PSC and reference PSC are 0.9896 and 0.9755, respectively. Although the exponential factor for Co 3 O 4 ‐PSC is a slightly larger than that of the reference PSC, both the values of α for reference and Co 3 O 4 ‐PSC are extremely close to 1, indicating the negligible bimolecular recombination in reference and Co 3 O 4 ‐PSC . In addition, the light intensity dependence of V oc can be investigated according to the following relation: Voc=nkTeαlntrue(italicItrue)+c, where k is the Boltzmann constant; T is absolute temperature; e refers to the elementary charge; the α and n are ideal factors related to recombination; c is a constant .…”
Section: Resultsmentioning
confidence: 99%