JOURNAL ARTICLE

Optical Properties of Two-Dimensional Perovskite Films\nof (C<sub>6</sub>H<sub>5</sub>C<sub>2</sub>H<sub>4</sub>NH<sub>3</sub>)<sub>2</sub>[PbI<sub>4</sub>] and (C<sub>6</sub>H<sub>5</sub>C<sub>2</sub>H<sub>4</sub>NH<sub>3</sub>)<sub>2</sub> (CH<sub>3</sub>NH<sub>3</sub>)<sub>2</sub>[Pb<sub>3</sub>I<sub>10</sub>]

Abstract

The\ntemperature dependence of absorption and photoluminescence\n(PL) spectroscopies were used to study the optical properties of 2D\nperovskite films, including <i>n</i> = 1 and 3 of (PEA)<sub>2</sub>(CH<sub>3</sub>NH<sub>3</sub>)<sub><i>n</i>−1</sub>[Pb<sub><i>n</i></sub>I<sub>3<i>n</i>+1</sub>] (PEA = C<sub>6</sub>H<sub>5</sub>(CH<sub>2</sub>)<sub>2</sub>NH<sub>3</sub>). In (PEA)<sub>2</sub>[Pb<sub>1</sub>I<sub>4</sub>] (PEPI),\nexcitons coupling to optical phonons with an average energy of ∼30\nmeV dominate the photophysics of absorption and PL. (PEA)<sub>2</sub>(CH<sub>3</sub>NH<sub>3</sub>)<sub>2</sub>[Pb<sub>3</sub>I<sub>10</sub>] (shortened as PMPI<sub>3</sub>), nominally prepared as <i>n</i> = 3, actually was a mixture of multiple layered perovskites\nwith various <i>n</i>. In absorption, a PMPI<sub>3</sub> film presents respective <i>n</i> materials’ excitonic\nfeatures, coupling to phonons with an average energy of ∼30\nmeV; in analyzing PL peaked singly at ∼1.6 eV and its width\nas a function of temperature, we found that PMPI<sub>3</sub> behaves\nlike PEPI at around 80 K but like 3D perovskite near room temperature,\nwith three times larger electron–phonon interaction strength\ncompared to that in PEPI.

Keywords:
Phonon Perovskite (structure) Absorption (acoustics) Coupling (piping) Absorption spectroscopy Energy (signal processing)

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