Temperature-Dependent Band Gap in Two-Dimensional Perovskites: Thermal Expansion Interaction and Electron–Phonon Interaction

Two-dimensional organic–inorganic perovskites have attracted considerable interest recently. Here, we present a systematic study of the temperature-dependent photoluminescence on phase pure (n-BA)2(MA) n−1Pb n I3n+1 (n = 1–5) and (iso-BA)2(MA) n−1Pb n I3n+1 (n = 1–3) microplates obtained by mechanic...

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Published inThe journal of physical chemistry letters Vol. 10; no. 10; pp. 2546 - 2553
Main Authors Wang, Shuai, Ma, Jiaqi, Li, Wancai, Wang, Jun, Wang, Haizhen, Shen, Hongzhi, Li, Junze, Wang, Jiaqi, Luo, Hongmei, Li, Dehui
Format Journal Article
LanguageEnglish
Published American Chemical Society 16.05.2019
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Summary:Two-dimensional organic–inorganic perovskites have attracted considerable interest recently. Here, we present a systematic study of the temperature-dependent photoluminescence on phase pure (n-BA)2(MA) n−1Pb n I3n+1 (n = 1–5) and (iso-BA)2(MA) n−1Pb n I3n+1 (n = 1–3) microplates obtained by mechanical exfoliation. The photoluminescence peak position gradually changes from a red-shift for n = 1 to a blue-shift for n = 5 with an increase in temperature in the (n-BA)2(MA) n−1Pb n I3n+1 (n = 1–5) series, while only a monotonous blue-shift has been observed for the (iso-BA)2(MA) n−1Pb n I3n+1 (n = 1–3) series, which can be attributed to the competition between the thermal expansion interaction and electron–phonon interaction. In the (n-BA)2(MA) n−1Pb n I3n+1 (n = 1–5) series, the thermal expansion interaction and electron–phonon interaction are both gradually enhanced and the former progressively dominates the latter from n = 1 to n = 5, resulting in the band gap versus temperature changing from a red-shift to a blue-shift. In contrast, both of these factors show a weaker layer thickness dependence, leading to the monotonous blue-shift in the (iso-BA)2(MA) n−1Pb n I3n+1 (n = 1–3) series.
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ISSN:1948-7185
1948-7185
DOI:10.1021/acs.jpclett.9b01011