Your browser doesn't support javascript.
loading
Single-Exciton Amplified Spontaneous Emission in Thin Films of CsPbX3 (X = Br, I) Perovskite Nanocrystals.
Navarro-Arenas, Juan; Suárez, Isaac; Chirvony, Vladimir S; Gualdrón-Reyes, Andrés F; Mora-Seró, Iván; Martínez-Pastor, Juan.
Afiliação
  • Navarro-Arenas J; Instituto de Ciencia de Materiales (ICMUV) , Universidad de Valencia , C/Catedrático José Beltrán, 2 , 46980 Paterna , Spain.
  • Suárez I; Instituto de Ciencia de Materiales (ICMUV) , Universidad de Valencia , C/Catedrático José Beltrán, 2 , 46980 Paterna , Spain.
  • Chirvony VS; ETSI Telecomunicación , Universidad Rey Juan Carlos , C/Camino del Molino s/n , 28943 Fuenlabrada , Spain.
  • Gualdrón-Reyes AF; Instituto de Ciencia de Materiales (ICMUV) , Universidad de Valencia , C/Catedrático José Beltrán, 2 , 46980 Paterna , Spain.
  • Mora-Seró I; Institute of Advanced Materials (INAM) , University Jaume I , Avenida de Vicent Sos Baynat, s/n , 12071 Castelló de la Plana , Castellón , Spain.
  • Martínez-Pastor J; Biofuels Lab-IBEAR, Faculty of Basic Sciences , University of Pamplona , Pamplona C.P. 543050 , Colombia.
J Phys Chem Lett ; 10(20): 6389-6398, 2019 Oct 17.
Article em En | MEDLINE | ID: mdl-31545904
ABSTRACT
CsPbX3 perovskite nanocrystals (PNCs) have emerged as an excellent material for stimulated emission purposes, with even more prospective applications than conventional colloidal quantum dots. However, a better understanding of the physical mechanisms responsible for amplified spontaneous emission (ASE) is required to achieve more ambitious targets (lasing under continuous wave optical or electrical excitation). Here, we establish the intrinsic mechanisms underlying ASE in PNCs of three different band gaps (CsPbBr3, CsPbBr1.5I1.5, and CsPbI3). Our characterization at cryogenic temperatures does not reveal any evidence of the biexciton mechanism in the formation of ASE. Instead, the measured shift toward long wavelengths of the ASE band is easily explained by the reabsorption in the PNC layer, which becomes stronger for thicker layers. In this way, the threshold of ASE is determined only by optical losses at a given geometry, which is the single-exciton mechanism responsible for ASE. Experimental results are properly reproduced by a physical model.

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2019 Tipo de documento: Article

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2019 Tipo de documento: Article