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A Nanojunction Polymer Photoelectrode for Efficient Charge Transport and Separation.
Ruan, Qiushi; Luo, Wenjun; Xie, Jijia; Wang, Yiou; Liu, Xu; Bai, Zhiming; Carmalt, Claire J; Tang, Junwang.
Afiliação
  • Ruan Q; Solar Energy & Advanced Materials Research Group, Department of Chemical Engineering, UCL, Torrington Place, London, WC1E 7JE, UK.
  • Luo W; Solar Energy & Advanced Materials Research Group, Department of Chemical Engineering, UCL, Torrington Place, London, WC1E 7JE, UK.
  • Xie J; Key Laboratory of Flexible Electronics (KLOFE) & Institute of Advanced Materials (IAM), Jiangsu National Synergetic Innovation Center for Advanced Materials (SICAM), Nanjing Tech University (NanjingTech), 30 South Puzhu Road, Nanjing, 211816, P.R. China.
  • Wang Y; Solar Energy & Advanced Materials Research Group, Department of Chemical Engineering, UCL, Torrington Place, London, WC1E 7JE, UK.
  • Liu X; Solar Energy & Advanced Materials Research Group, Department of Chemical Engineering, UCL, Torrington Place, London, WC1E 7JE, UK.
  • Bai Z; Solar Energy & Advanced Materials Research Group, Department of Chemical Engineering, UCL, Torrington Place, London, WC1E 7JE, UK.
  • Carmalt CJ; The school of material science and engineering, Beihang University, No.37 Xueyuan Road, Haidian district, Beijing, China.
  • Tang J; Department of Chemistry, UCL, 20 Gordon Street, London, WC1H 0AJ, UK.
Angew Chem Int Ed Engl ; 56(28): 8221-8225, 2017 07 03.
Article em En | MEDLINE | ID: mdl-28520233
ABSTRACT
A metal-free photoanode nanojunction architecture, composed of B-doped carbon nitride nanolayer and bulk carbon nitride, was fabricated by a one-step approach. This type of nanojunction (s-BCN) overcomes a few intrinsic drawbacks of carbon nitride film (severe bulk charge recombination and slow charge transfer). The top layer of the nanojunction has a depth of ca. 100 nm and the bottom layer is ca. 900 nm. The nanojunction photoanode results into a 10-fold higher photocurrent than bulk graphitic carbon nitride (G-CN) photoanode, with a record photocurrent density of 103.2 µA cm-2 at 1.23 V vs. RHE under one sun irradiation and an extremely high incident photon-to-current efficiency (IPCE) of ca. 10 % at 400 nm. Electrochemical impedance spectroscopy, Mott-Schottky plots, and intensity-modulated photocurrent spectroscopy show that such enhancement is mainly due to the mitigated deep trap states, a more than 10 times faster charge transfer rate and nearly three times higher conductivity due to the nanojunction architecture.
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Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2017 Tipo de documento: Article

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2017 Tipo de documento: Article