2021
DOI: 10.1021/acs.jpclett.1c02072
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Transformation between the Dark and Bright Self-Trapped Excitons in Lead-Free Double-Perovskite Cs2NaBiCl6 under Pressure

Abstract: Understanding the relationships between the structure and the properties in lead-free double perovskites is significant for their applications in the optoelectronic field. Here the nonluminous Cs2NaBiCl6 crystal exhibits an unexpected broadband dual-color emission as the external pressure is increased to 6.77 GPa. The emission intensity is remarkably enhanced with further compression to 8.50 GPa. By analyzing the results of in situ high-pressure experiments and the density functional theory, we conclude that t… Show more

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Cited by 30 publications
(36 citation statements)
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“…14−16 In Mn 2+ -doped double perovskite systems, most of the energy transfer processes usually take place from the STE state of the double perovskite to Mn 2+ rather than directly from free electrons to Mn 2+ , 14,17,18 which would generate a pronounced energy loss caused by the inevitable defects between the host and doped states. 19,20 Therefore, realizing the direct energy transfer between the host and dopant is crucial for enhancing the PL efficiency of double perovskites.…”
mentioning
confidence: 99%
“…14−16 In Mn 2+ -doped double perovskite systems, most of the energy transfer processes usually take place from the STE state of the double perovskite to Mn 2+ rather than directly from free electrons to Mn 2+ , 14,17,18 which would generate a pronounced energy loss caused by the inevitable defects between the host and doped states. 19,20 Therefore, realizing the direct energy transfer between the host and dopant is crucial for enhancing the PL efficiency of double perovskites.…”
mentioning
confidence: 99%
“…For example, the two Pb 2+ was replaced into [Na + + Bi 3+ ] and [Ag + + Bi 3+ ], generating two cubic double perovskites Cs 2 NaBiCl 6 and Cs 2 AgBiCl 6 (Figure 1). 42,43 First, the DFT calculations confirm the intricate band gap evolutions of cubic Cs 2 NaBiCl 6 and cubic Cs 2 AgBiCl 6 observed in photoluminescence spectra under pressure 29,30 (Figure 2). As shown in Figure 2c and d, the DFT band gap of Cs 2 NaBiCl 6 gradually increases to 0.03 eV while pressure changes from 1 atm to 5 GPa, whereas the band gap of Cs 2 AgBiCl 6 decreases to as large as 0.37 eV in the same pressure range.…”
Section: ■ Computational Detailsmentioning
confidence: 62%
“…28 By applying pressure, recent studies successfully reduced the band gap of Cs 2 AgBiBr 6 from ∼2.2 to 1.7 eV 27 and regulated the photoluminescence emission range in Cs 2 AgBiCl 6 and Cs 2 NaBiCl 6 . 29,30 Interestingly, the band gap of Cs 2 NaBiCl 6 increases with pressure up to ∼5 GPa, whereas the band gaps of Cs 2 AgBiCl 6 /Cs 2 AgBiBr 6 decrease with pressure in the studied range (<5 GPa for Cs 2 AgBiCl 6 or <3 GPa for Cs 2 AgBiBr 6 ). Then, they transform into a tetrahedral structure at higher pressure.…”
Section: ■ Introductionmentioning
confidence: 91%
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“…The Letter by Li et al + ions in the growth of single ice crystals. The Letter by Jiang et al 12 reports the luminescence properties of lead-free double-perovskite Cs 2 NaBiCl 6 crystals under high pressure. The Letter by Wang et al 13 reports the relationship between the delocalization of metal cluster cores in tin clusters as a potential third-order nonlinear optical (NLO) material.…”
mentioning
confidence: 99%