2020
DOI: 10.1038/s41467-020-15451-1
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Reduced-dimensional perovskite photovoltaics with homogeneous energy landscape

Abstract: Reduced-dimensional (quasi-2D) perovskite materials are widely applied for perovskite photovoltaics due to their remarkable environmental stability. However, their device performance still lags far behind traditional three dimensional perovskites, particularly high open circuit voltage (V oc) loss. Here, inhomogeneous energy landscape is pointed out to be the sole reason, which introduces extra energy loss, creates band tail states and inhibits minority carrier transport. We thus propose to form homogeneous en… Show more

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Cited by 234 publications
(246 citation statements)
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“…Under bottom excitation, the evolution of the reducing bleach signals assigned to n = 3, 4, and 5 phases is accompanied by the enhanced bleach signal at n ≈ ∞ phase within the delay time of 300 ps (see Figure 3 a,b), suggesting that the electrons can spontaneously transfer from the smaller n to n ≈ ∞ phases in both the control and aqueous precursor‐based films. [ 35,38,39 ] This process is also observed in the corresponding films under front excitation at early delay time (within 40 ps, see Figure 3c,d), corresponding to the penetration of photons through the n ≈ ∞ phase and resultant charge transfers to the low energy gap phases. It is noteworthy that the TA spectra of control film display multiple higher energy bleach signals at n = 3, 4, and 5 phases under front excitation.…”
Section: Figurementioning
confidence: 60%
“…Under bottom excitation, the evolution of the reducing bleach signals assigned to n = 3, 4, and 5 phases is accompanied by the enhanced bleach signal at n ≈ ∞ phase within the delay time of 300 ps (see Figure 3 a,b), suggesting that the electrons can spontaneously transfer from the smaller n to n ≈ ∞ phases in both the control and aqueous precursor‐based films. [ 35,38,39 ] This process is also observed in the corresponding films under front excitation at early delay time (within 40 ps, see Figure 3c,d), corresponding to the penetration of photons through the n ≈ ∞ phase and resultant charge transfers to the low energy gap phases. It is noteworthy that the TA spectra of control film display multiple higher energy bleach signals at n = 3, 4, and 5 phases under front excitation.…”
Section: Figurementioning
confidence: 60%
“…In general, defects in the crystal structure cause PL quenching, which leads to a shortened PL lifetime of photogenerated carriers in the absorber layer. [ 39 ] Here, prolonged PL lifetime of photogenerated carriers may come from a reduction of Shockley–Read–Hall (SRH) recombination via bulk defects in the MAPbI 3 –SDBS film, and indicates a lower defect concentration for MAPbI 3 –SDBS film, [ 59,60 ] further suggesting that the SDBS passivation dramatically inhibits the nonradiative recombination. To more accurately quantitatively assess the trap‐state density ( N t ) of different perovskite films, we fabricated the electron‐only devices with the structure of FTO/SnO 2 /perovskite/PCBM/Au, and measured the dark current–voltage curves of the space charge‐limited current (SCLC) as a function of the different bias voltages, as shown in Figure 3f.…”
Section: Resultsmentioning
confidence: 99%
“…[69] Further, the electronic coupling between inorganic layers also has a non-negligible effect on the distance between layers. [70][71][72][73] However, the dielectric constant of organic materials is significantly smaller than that of inorganic materials, which leads to the obvious quantum confinement effect in 2D perovskites. [74] This also indicates that the carrier transport path is limited in the inorganic layer.…”
Section: Natural Quantum Well Structurementioning
confidence: 99%