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Tunable White-Light Emission in Single-Cation-Templated Three-Layered 2D Perovskites (CH 3 CH 2 NH 3 ) 4 Pb 3 Br 10-x Cl x .

Authors :
Mao L
Wu Y
Stoumpos CC
Traore B
Katan C
Even J
Wasielewski MR
Kanatzidis MG
Source :
Journal of the American Chemical Society [J Am Chem Soc] 2017 Aug 30; Vol. 139 (34), pp. 11956-11963. Date of Electronic Publication: 2017 Aug 16.
Publication Year :
2017

Abstract

Two-dimensional (2D) hybrid halide perovskites come as a family (B) <subscript>2</subscript> (A) <subscript>n-1</subscript> Pb <subscript>n</subscript> X <subscript>3n+1</subscript> (B and A= cations; X= halide). These perovskites are promising semiconductors for solar cells and optoelectronic applications. Among the fascinating properties of these materials is white-light emission, which has been mostly observed in single-layered 2D lead bromide or chloride systems (n = 1), where the broad emission comes from the transient photoexcited states generated by self-trapped excitons (STEs) from structural distortion. Here we report a multilayered 2D perovskite (n = 3) exhibiting a tunable white-light emission. Ethylammonium (EA <superscript>+</superscript> ) can stabilize the 2D perovskite structure in EA <subscript>4</subscript> Pb <subscript>3</subscript> Br <subscript>10-x</subscript> Cl <subscript>x</subscript> (x = 0, 2, 4, 6, 8, 9.5, and 10) with EA <superscript>+</superscript> being both the A and B cations in this system. Because of the larger size of EA, these materials show a high distortion level in their inorganic structures, with EA <subscript>4</subscript> Pb <subscript>3</subscript> Cl <subscript>10</subscript> having a much larger distortion than that of EA <subscript>4</subscript> Pb <subscript>3</subscript> Br <subscript>10</subscript> , which results in broadband white-light emission of EA <subscript>4</subscript> Pb <subscript>3</subscript> Cl <subscript>10</subscript> in contrast to narrow blue emission of EA <subscript>4</subscript> Pb <subscript>3</subscript> Br <subscript>10</subscript> . The average lifetime of the series decreases gradually from the Cl end to the Br end, indicating that the larger distortion also prolongs the lifetime (more STE states). The band gap of EA <subscript>4</subscript> Pb <subscript>3</subscript> Br <subscript>10-x</subscript> Cl <subscript>x</subscript> ranges from 3.45 eV (x = 10) to 2.75 eV (x = 0), following Vegard's law. First-principles density functional theory calculations (DFT) show that both EA <subscript>4</subscript> Pb <subscript>3</subscript> Cl <subscript>10</subscript> and EA <subscript>4</subscript> Pb <subscript>3</subscript> Br <subscript>10</subscript> are direct band gap semiconductors. The color rendering index (CRI) of the series improves from 66 (EA <subscript>4</subscript> Pb <subscript>3</subscript> Cl <subscript>10</subscript> ) to 83 (EA <subscript>4</subscript> Pb <subscript>3</subscript> Br <subscript>0.5</subscript> Cl <subscript>9.5</subscript> ), displaying high tunability and versatility of the title compounds.

Details

Language :
English
ISSN :
1520-5126
Volume :
139
Issue :
34
Database :
MEDLINE
Journal :
Journal of the American Chemical Society
Publication Type :
Academic Journal
Accession number :
28745881
Full Text :
https://doi.org/10.1021/jacs.7b06143