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Temperature-dependent excitonic emission characteristics of highly crystallized carbon nitride nanosheets.
Wang, Yue; Zhang, Guodi; Zhao, Min; Qi, Hongbo; Gao, Tianqi; An, Limin; Sun, Jianhui.
Afiliación
  • Wang Y; College of Physical Science and Technology, Heilongjiang University, Harbin 150080, People's Republic of China.
  • Zhang G; College of Physical Science and Technology, Heilongjiang University, Harbin 150080, People's Republic of China.
  • Zhao M; College of Physical Science and Technology, Heilongjiang University, Harbin 150080, People's Republic of China.
  • Qi H; College of Physical Science and Technology, Heilongjiang University, Harbin 150080, People's Republic of China.
  • Gao T; College of Physical Science and Technology, Heilongjiang University, Harbin 150080, People's Republic of China.
  • An L; College of Physical Science and Technology, Heilongjiang University, Harbin 150080, People's Republic of China.
  • Sun J; College of Physical Science and Technology, Heilongjiang University, Harbin 150080, People's Republic of China.
Nanotechnology ; 35(30)2024 May 07.
Article en En | MEDLINE | ID: mdl-38604151
ABSTRACT
Highly-crystallized carbon nitride (HCCN) nanosheets exhibit significant potential for advancements in the field of photoelectric conversion. However, to fully exploit their potential, a thorough understanding of the fundamental excitonic photophysical processes is crucial. Here, the temperature-dependent excitonic photoluminescence (PL) of HCCN nanosheets and amorphous polymeric carbon nitride (PCN) is investigated using steady-state and time-resolved PL spectroscopy. The exciton binding energy of HCCN is determined to be 109.26 meV, lower than that of PCN (207.39 meV), which is attributed to the ordered stacking structure of HCCN with a weaker Coulomb interaction between electrons and holes. As the temperature increases, a noticeable reduction in PL lifetime is observed on both the HCCN and PCN, which is ascribed to the thermal activation of carrier trapping by the enhanced electron-phonon coupling effect. The thermal activation energy of HCCN is determined to be 102.9 meV, close to the value of PCN, due to their same band structures. Through wavelength-dependent PL dynamics analysis, we have identified the PL emission of HCCN as deriving from the transitionsσ*-LP,π*-π, andπ*-LP, where theπ*-LP transition dominants the emission because of the high excited state density of the LP state. These results demonstrate the impact of high-crystallinity on the excitonic emission of HCCN materials, thereby expanding their potential applications in the field of photoelectric conversion.
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Texto completo: 1 Colección: 01-internacional Base de datos: MEDLINE Idioma: En Revista: Nanotechnology Año: 2024 Tipo del documento: Article

Texto completo: 1 Colección: 01-internacional Base de datos: MEDLINE Idioma: En Revista: Nanotechnology Año: 2024 Tipo del documento: Article