Premium
Understanding the Electronic Structures of Graphene Quantum Dot Physisorption and Chemisorption onto the TiO 2 (110) Surface: A First‐Principles Calculation
Author(s) -
Long Run
Publication year - 2013
Publication title -
chemphyschem
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.016
H-Index - 140
eISSN - 1439-7641
pISSN - 1439-4235
DOI - 10.1002/cphc.201200882
Subject(s) - physisorption , chemisorption , graphene , chemistry , chemical physics , van der waals force , materials science , adsorption , nanotechnology , molecule , organic chemistry
We investigated the interfacial electronic structure and charge transfer properties of graphene quantum dot (GQD) physisorption and chemisorption on the TiO 2 (110) surface from density functional theory calculations. The simulations show that a slight charge transfer occurs in physisorption case while a significant charge transfer takes place in chemisorption configuration. We present a detailed comparison of the similarities and differences between the electronic structures. The similarities originate from the positive work function difference in both the physisorption and chemisorption configurations, which is able to drive electron transfer from GQD into TiO 2 , leading to charge separation across the GQD–TiO 2 interface. The differences stem from the interaction between the GQD and TiO 2 substrate. For example, GQD bounds to TiO 2 surface through van der Waals interactions in the case of physisorption. In the chemisorption configuration, however, there exists strong covalent bonding between them. This leads to much more efficient charge separation for chemisorption than for physisorption. Furthermore, the GQD–TiO 2 composites show large band‐gap narrowing that could extend the optical absorption edge into the visible‐light region. This should imply that chemisorbed GQDs produce a composite with better photocatalytic and photovoltaic performance than composites formed through physisorption.