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      Modulation of interfacial charge transfer by self-assembly of single-layer graphene enwrapped one-dimensional semiconductors toward photoredox catalysis

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          Abstract

          A progressive layer-by-layer self-assembly strategy has been developed to construct a graphene-wrapped and WO 3 nanorods-coupled TiO 2 nanobelts photocatalyst, in which a highly efficient cascade electron transfer pathway was judiciously built.

          Abstract

          In recent years, the exquisite modulation of the transport of photogenerated electron–hole charge carriers has constituted a long-standing challenge. To this end, herein, a spatially hierarchical single-layer graphene (GR)–wrapped and WO 3 nanorods (NRs)–coupled TiO 2 nanobelts (TNBs) ternary nano-architecture (TNBs/WO 3 NRs/GR), as a conceptual platform, has been progressively designed via a facile and green layer-by-layer assembly strategy based on pronounced electrostatic interaction. It was remarkable to find that the interfacial charge transfer of a TNBs/WO 3 NRs/GR ternary heterostructure can be finely modulated by interfacial architectural engineering, thus contributing to its significantly improved photoredox performance, including photocatalytic oxidation of organic pollutants and reduction of heavy metal ions, in comparison with single and binary counterparts. The construction of highly efficient cascade electron transfer pathways at the interface is responsible for the enhancement in photoactivities of a ternary heterostructure, which is afforded by intimately intercalating WO 3 NRs in the interfacial domains of TNBs and GR. In this unique ternary nano-architecture, the WO 3 NRs ingredient serves as an efficient interfacial charge transfer mediator and GR serves as an electron transporter and collector to conspicuously trigger a cascade electron relay from TNBs to GR, thereby expediting the efficacious charge transfer, prolonging the lifetime of photogenerated electron–hole pairs, and resulting in the significantly enhanced photoredox activities of the TNBs/WO 3 NRs/GR heterostructure. In addition, the predominant active species responsible for the photoredox process were determined and the underlying photocatalytic mechanism was delineated.

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          Most cited references56

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          Is Open Access

          The rise of graphene

          Graphene is a rapidly rising star on the horizon of materials science and condensed matter physics. This strictly two-dimensional material exhibits exceptionally high crystal and electronic quality and, despite its short history, has already revealed a cornucopia of new physics and potential applications, which are briefly discussed here. Whereas one can be certain of the realness of applications only when commercial products appear, graphene no longer requires any further proof of its importance in terms of fundamental physics. Owing to its unusual electronic spectrum, graphene has led to the emergence of a new paradigm of 'relativistic' condensed matter physics, where quantum relativistic phenomena, some of which are unobservable in high energy physics, can now be mimicked and tested in table-top experiments. More generally, graphene represents a conceptually new class of materials that are only one atom thick and, on this basis, offers new inroads into low-dimensional physics that has never ceased to surprise and continues to provide a fertile ground for applications.
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            Two-Dimensional Gas of Massless Dirac Fermions in Graphene

            Electronic properties of materials are commonly described by quasiparticles that behave as non-relativistic electrons with a finite mass and obey the Schroedinger equation. Here we report a condensed matter system where electron transport is essentially governed by the Dirac equation and charge carriers mimic relativistic particles with zero mass and an effective "speed of light" c* ~10^6m/s. Our studies of graphene - a single atomic layer of carbon - have revealed a variety of unusual phenomena characteristic of two-dimensional (2D) Dirac fermions. In particular, we have observed that a) the integer quantum Hall effect in graphene is anomalous in that it occurs at half-integer filling factors; b) graphene's conductivity never falls below a minimum value corresponding to the conductance quantum e^2/h, even when carrier concentrations tend to zero; c) the cyclotron mass m of massless carriers with energy E in graphene is described by equation E =mc*^2; and d) Shubnikov-de Haas oscillations in graphene exhibit a phase shift of pi due to Berry's phase.
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              Graphene: Status and Prospects

              A. K. Geim (2010)
              Graphene is a wonder material with many superlatives to its name. It is the thinnest material in the universe and the strongest ever measured. Its charge carriers exhibit giant intrinsic mobility, have the smallest effective mass (it is zero) and can travel micrometer-long distances without scattering at room temperature. Graphene can sustain current densities 6 orders higher than copper, shows record thermal conductivity and stiffness, is impermeable to gases and reconciles such conflicting qualities as brittleness and ductility. Electron transport in graphene is described by a Dirac-like equation, which allows the investigation of relativistic quantum phenomena in a bench-top experiment. What are other surprises that graphene keeps in store for us? This review analyses recent trends in graphene research and applications, and attempts to identify future directions in which the field is likely to develop.
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                Author and article information

                Journal
                JMCAET
                Journal of Materials Chemistry A
                J. Mater. Chem. A
                Royal Society of Chemistry (RSC)
                2050-7488
                2050-7496
                2017
                2017
                : 5
                : 45
                : 23681-23693
                Affiliations
                [1 ]College of Materials Science and Engineering
                [2 ]Fuzhou University
                [3 ]Fuzhou
                [4 ]People's Republic of China
                Article
                10.1039/C7TA08415C
                15b5857f-e22d-461d-afff-93868ea45a40
                © 2017

                http://rsc.li/journals-terms-of-use

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