Hostname: page-component-89b8bd64d-sd5qd Total loading time: 0 Render date: 2026-05-09T23:47:01.431Z Has data issue: false hasContentIssue false

Modifying oxide nanomaterials' properties by hydrogenation

Published online by Cambridge University Press:  09 September 2016

Xiaodong Yan
Affiliation:
Department of Chemistry, University of Missouri—Kansas City, Kansas City, MO 64110, USA
Lihong Tian
Affiliation:
Department of Chemistry, University of Missouri—Kansas City, Kansas City, MO 64110, USA Hubei Collaborative Innovation Center for Advanced Organochemical Materials, Ministry of Education Key Laboratory for the Synthesis and Applications of Organic Functional Molecules, Hubei University, Wuhan 430062, China
Xinyu Tan
Affiliation:
College of Materials and Chemical Engineering, Hubei Provincial Collaborative Innovation Center for New Energy Microgrid, China Three Gorges University, Yichang 443002, China
Minjie Zhou
Affiliation:
School of Chemistry and Chemical Engineering, Hunan Institute of Science and Technology, Yueyang 414000, China
Lei Liu
Affiliation:
State Key Laboratory of Luminescence and Applications, Changchun Institute of Optics, Fine Mechanics and Physics, Chinese Academy of Sciences, Changchun 130033, China
Xiaobo Chen*
Affiliation:
Department of Chemistry, University of Missouri—Kansas City, Kansas City, MO 64110, USA
*
Address all correspondence to Xiaobo Chen at chenxiaobo@umkc.edu

Abstract

Nanomaterials have been intensively studied over the past decades with many advantages over traditional bulk materials in many applications. Nanomaterials' properties are largely governed by their chemical compositions, sizes, shapes, dimensions, morphologies and structures, which are primarily controlled with the chemical and/or physical fabrication methods and processes. This prospective will highlight recent progress on the modifications of oxide nanomaterials' properties by hydrogenation, namely heat treatment under hydrogen or hydrogen plasma environment, for various applications.

Information

Type
Functional Oxides Prospective Articles
Copyright
Copyright © Materials Research Society 2016 
Figure 0

Figure 1. A brief summary of the characteristics of oxide nanomaterials after hydrogenation and the related applications.

Figure 1

Figure 2. Illustration of some possible scenarios of the chemical composition changes for oxide materials after hydrogenation treatments.

Figure 2

Figure 3. (a) A schematic illustration of the lattice and electronic structures of hydrogenated black TiO2, (b) Digital pictures of white and hydrogenated black TiO2, (c) HRTEM image of white TiO2, (d) HRTEM image of white TiO2, (e) UV-vis and (f) VB-XPS spectra of white and hydrogenated black TiO2. Reproduced with permission from Ref. 4, Copyright 2011 AAAS.

Figure 3

Figure 4. Photocatalytic H2 production under open circuit conditions in methanol/water (50/50 vol %) with TiO2 nanotubes and nanorods treated in different atmospheres under AM1.5 (100 mW/cm2) illumination.[32] Air, heat treatment in air at 450 °C; Ar, heat treatment in pure argon at 500 °C; Ar/H2, heat treatment in H2/Ar (5 vol %) at 500 °C; HP-H2, heat treatment in H2 at 20 bar at 500 °C; heat treatment in H2 at 20 bar at 200 °C for 5 days (following Sci Ref. 4).[32] Reprinted with permission from Ref. 32. Copyright 2014, American Chemical Society.

Figure 4

Figure 5. (a) Cyclic voltammetry profiles of the hydrogenated (H-TiO2) and pure (A-TiO2) anatase microspheres at a scan rate of 0.5 mV/s. Galvanostatic discharge–charge profiles of the (b) H-TiO2 and (c) A-TiO2 microspheres at various rates. (d) Comparison of the rate performance of the H-TiO2 and A-TiO2 microspheres.[39] Reprinted with permission from Ref. 39. Copyright 2013 The Royal Society of Chemistry.

Figure 5

Figure 6. (a) The mechanism of collective interfacial polarization amplified microwave absorption (CIPAMA) of hydrogenated TiO2 nanoparticles.[77] The collective movements of interfacial dipoles (CMID) at the anatase/rutile and crystalline/disordered interfaces amplify the response to the incoming electromagnetic field and thus induce enhanced microwave absorption performance. The positions of the electronic band structure of the disordered layer are assumed to lie between those of anatase and rutile phases. CBE: conduction band edge, VBE: valence band edge. Reprinted with permission from Ref. 77. Copyright 2013 Wiley-VCH. (b) Reflection loss of pristine and hydrogenated TiO2 nanocrystals.[78] Reprinted with permission from Ref. 78. Copyright 2014 Materials Research Society.

Figure 6

Figure 7. (a) Schematic illustration of the hydrogenation-induced structural change from NixCeO2+x to Ni/CeO2 on carbon nanotubes. (b) The electrochemical polarization curves for hydrogen evolution reactions on NixCeO2+x-CNT, Ni/CeO2-CNT, Ni-CNT, and Pt/C electrodes. CNT: carbon nanotube.[94] Reprinted with permission from Ref. 94. Copyright 2015, American Chemical Society.

Figure 7

Figure 8. (a) SEM and (b, c) TEM images of hydrogenated Ni/NiO crystalline/amorphous core/shell nanosheets.[106] Reprinted with permission from Ref. 106. Copyright 2015, Elsevier.

Figure 8

Figure 9. (a) SEM and (b, c) TEM images of hydrogenated Co/Co3O4 crystalline/amorphous core/shell nanosheets, (d) The electrochemical polarization curves for hydrogen evolution reactions on Ni, Co3O4, Co/Co3O4, and Pt/C.[107] Reprinted with permission from Ref. 107. Copyright 2015, American Chemical Society.