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Development of Cu-In-Ga-S quantum dots with a narrow emission peak for red electroluminescence.
Jiang, Chang; Tozawa, Makoto; Akiyoshi, Kazutaka; Kameyama, Tatsuya; Yamamoto, Takahisa; Motomura, Genichi; Fujisaki, Yoshihide; Uematsu, Taro; Kuwabata, Susumu; Torimoto, Tsukasa.
Afiliação
  • Jiang C; Graduate School of Engineering, Nagoya University, Chikusa-ku, Nagoya 464-8603, Japan.
  • Tozawa M; Graduate School of Engineering, Nagoya University, Chikusa-ku, Nagoya 464-8603, Japan.
  • Akiyoshi K; Graduate School of Engineering, Nagoya University, Chikusa-ku, Nagoya 464-8603, Japan.
  • Kameyama T; Graduate School of Engineering, Nagoya University, Chikusa-ku, Nagoya 464-8603, Japan.
  • Yamamoto T; Graduate School of Engineering, Nagoya University, Chikusa-ku, Nagoya 464-8603, Japan.
  • Motomura G; Science and Technology Research Laboratories, Japan Broadcasting Corporation (NHK), Setagaya-ku, Tokyo 157-8510, Japan.
  • Fujisaki Y; Department of Applied Chemistry, Graduate School of Engineering, Osaka University, Suita, Osaka 565-0871, Japan.
  • Uematsu T; Science and Technology Research Laboratories, Japan Broadcasting Corporation (NHK), Setagaya-ku, Tokyo 157-8510, Japan.
  • Kuwabata S; Department of Applied Chemistry, Graduate School of Engineering, Osaka University, Suita, Osaka 565-0871, Japan.
  • Torimoto T; Innovative Catalysis Science Division, Institute for Open and Transdisciplinary Research Initiatives (ICS-OTRI), Osaka University, Suita, Osaka 565-0871, Japan.
J Chem Phys ; 158(16)2023 Apr 28.
Article em En | MEDLINE | ID: mdl-37096856
Narrowing the emission peak width and adjusting the peak position play a key role in the chromaticity and color accuracy of display devices with the use of quantum dot light-emitting diodes (QD-LEDs). In this study, we developed multinary Cu-In-Ga-S (CIGS) QDs showing a narrow photoluminescence (PL) peak by controlling the Cu fraction, i.e., Cu/(In+Ga), and the ratio of In to Ga composing the QDs. The energy gap of CIGS QDs was enlarged from 1.74 to 2.77 eV with a decrease in the In/(In+Ga) ratio from 1.0 to 0. The PL intensity was remarkably dependent on the Cu fraction, and the PL peak width was dependent on the In/(In+Ga) ratio. The sharpest PL peak at 668 nm with a full width at half maximum (fwhm) of 0.23 eV was obtained for CIGS QDs prepared with ratios of Cu/(In+Ga) = 0.3 and In/(In+Ga) = 0.7, being much narrower than those previously reported with CIGS QDs, fwhm of >0.4 eV. The PL quantum yield of CIGS QDs, 8.3%, was increased to 27% and 46% without a PL peak broadening by surface coating with GaSx and Ga-Zn-S shells, respectively. Considering a large Stokes shift of >0.5 eV and the predominant PL decay component of ∼200-400 ns, the narrow PL peak was assignable to the emission from intragap states. QD-LEDs fabricated with CIGS QDs surface-coated with GaSx shells showed a red color with a narrow emission peak at 688 nm with a fwhm of 0.24 eV.

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Ano de publicação: 2023 Tipo de documento: Article

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Ano de publicação: 2023 Tipo de documento: Article