2019
DOI: 10.1021/acs.jpclett.9b00876
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Equal Footing of Thermal Expansion and Electron–Phonon Interaction in the Temperature Dependence of Lead Halide Perovskite Band Gaps

Abstract: Lead halide perovskites, which are causing a paradigm shift in photovoltaics, exhibit an atypical temperature dependence of the fundamental gap: it decreases in energy with decreasing temperature. Reports ascribe such a behavior to a strong electron-phonon renormalization

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Cited by 79 publications
(85 citation statements)
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“…This appears to be a general trend in metal halide perovskites, [ 16,24,29,31,32 ] in frank contrast with the flat plateau exhibited by the gap of most tetrahedrally bonded semiconductors. [ 33 ] It turns out that such unusual temperature‐induced renormalization of the band gap in the perovskites is partly due to a peculiar electron–phonon interaction, [ 34 ] determined by the coupling to the very low‐frequency modes of the inorganic cage. [ 35–37 ]…”
Section: Resultsmentioning
confidence: 99%
“…This appears to be a general trend in metal halide perovskites, [ 16,24,29,31,32 ] in frank contrast with the flat plateau exhibited by the gap of most tetrahedrally bonded semiconductors. [ 33 ] It turns out that such unusual temperature‐induced renormalization of the band gap in the perovskites is partly due to a peculiar electron–phonon interaction, [ 34 ] determined by the coupling to the very low‐frequency modes of the inorganic cage. [ 35–37 ]…”
Section: Resultsmentioning
confidence: 99%
“…It should be noted that the red‐shifted PL does not necessarily mean an increased population of in‐band states or impurities (as those generally serve a nonradiative recombination center) but a characteristic of MAPbI 3 perovskites identified in both poly‐ or mono‐crystalline forms. [ 31,33–35 ] The indicated reduction of E g at lower T may partially contribute to the enlargement of J SC (provided that the absorption coefficient of tetragonal MAPbI 3 is roughly T ‐invariable [ 33 ] ). Given the reduced E g (with reducing T ), the saturation trend of V OC at lower T may also be reconciled.…”
Section: Resultsmentioning
confidence: 99%
“…Computational modeling has attributed the increase in bandgap upon temperature increase to electron-phonon coupling and thermal expansion. 197,207,208 Interestingly, we recently observed a ~30 meV red shift in the PL spectrum of MAPbI 3 across the tetragonal-cubic transition when MAPbI 3 crystals were nanoconfined in the ~20 -250 diameter pores of AAO (Figure 9), 150 opposite of the trend observed in bulk crystals. By increasing the surface area-tovolume ratio of these crystals, nanoconfinement shifted the relative Gibbs free energies of the , , and  phases such that the - transition temperature was lowered from ~330 K to between 170 -200 K. At these lower temperatures, thermal fluctuations in the M-X framework are likely suppressed, resulting in a narrowing of the bandgap upon transitioning to the cubic phase with I-Pb-I angles of 180 o .…”
Section: Materials Advances Accepted Manuscriptmentioning
confidence: 90%