2023
DOI: 10.1002/aenm.202300382
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Minimized Energy Loss at the Buried Interface of p‐i‐n Perovskite Solar Cells via Accelerating Charge Transfer and Forming p–n Homojunction

Abstract: The energy loss (Eloss) aroused by inefficient charge transfer and large energy level offset at the buried interface of p‐i‐n perovskite solar cells (PVSCs) limits their development. In this work, a BF4− anion‐assisted molecular doping (AMD) strategy is first proposed to improve the charge transfer capability of hole transport layers (HTLs) and reduce the energy level offset at the buried interface of PVSCs. The AMD strategy improves the carrier mobility and density of poly[bis(4‐phenyl) (2,4,6‐trimethylphenyl… Show more

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Cited by 20 publications
(9 citation statements)
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“…When n approaches 1, it indicates that bimolecular recombination plays a dominant role, whereas trap-assisted recombination is inhibited, leading to higher FF and higher PCE. When n approaches 2, it indicates that bimolecular recombination is inhibited and trap-assisted recombination plays a dominant role, resulting in lower FF and lower PCE. , As shown in Figure e and Figure S11e, the n values of devices with ZrSe 2 , ZrSe 2 :PTSA, PEDOT:PSS, and ITO HTLs are 1.28, 1.24, 1.18, and 1.44, respectively. Among them, the n of the device with ZrSe 2 :PTSA HTL is lower than that of the device with the original ZrSe 2 HTL, indicating that the trap-assisted recombination of ZrSe 2 is more effectively inhibited after modification with PTSA.…”
Section: Resultsmentioning
confidence: 97%
“…When n approaches 1, it indicates that bimolecular recombination plays a dominant role, whereas trap-assisted recombination is inhibited, leading to higher FF and higher PCE. When n approaches 2, it indicates that bimolecular recombination is inhibited and trap-assisted recombination plays a dominant role, resulting in lower FF and lower PCE. , As shown in Figure e and Figure S11e, the n values of devices with ZrSe 2 , ZrSe 2 :PTSA, PEDOT:PSS, and ITO HTLs are 1.28, 1.24, 1.18, and 1.44, respectively. Among them, the n of the device with ZrSe 2 :PTSA HTL is lower than that of the device with the original ZrSe 2 HTL, indicating that the trap-assisted recombination of ZrSe 2 is more effectively inhibited after modification with PTSA.…”
Section: Resultsmentioning
confidence: 97%
“…Due to the weak bonding in Pb−I bonds, iodine ions are easy to migrate under the influence of environmental stress, which will leave a large number of donor-type V I vacancy defects on the surface of the perovskite film, leading to a more n-type perovskite surface. 7 Therefore, PT molecules can regulate and passivate V I defects to make the energy-level structure of the perovskite surface shift downward. Compared with the control film, the CBM of the PT-modified perovskite film is closer to the lowest unoccupied molecular orbital level of the PCBM ETL (−4.20 eV), indicating a smaller electron transport barrier.…”
Section: Resultsmentioning
confidence: 99%
“…Based on the linear intersection method and band gap values, the conduction band minimum (CBM)/valence band maximum (VBM) values of the control and PT-modified perovskite films can be estimated as −4.04/–5.59 and −4.12/–5.66 eV, respectively. , Therefore, the energy-level diagrams of the control and PT-modified perovskite films are revealed in Figure f, and the detailed parameter values are summarized in Table S1. Due to the weak bonding in Pb–I bonds, iodine ions are easy to migrate under the influence of environmental stress, which will leave a large number of donor-type V I vacancy defects on the surface of the perovskite film, leading to a more n-type perovskite surface . Therefore, PT molecules can regulate and passivate V I defects to make the energy-level structure of the perovskite surface shift downward.…”
Section: Resultsmentioning
confidence: 99%
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“…The relationship between J sc and light intensity can be expressed by the formula J sc ∝ I α . 40 The closer the value of α tends to 1, the more likely the bimolecular recombination probability of OSCs tends to be 0. The fitted J sc –light intensity dependence curve is shown in Fig.…”
Section: Calculation Detailsmentioning
confidence: 99%