2013
DOI: 10.1039/c3tc30845f
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An edge-contacted pn-heterojunction of a p-SWCNT/n-WO3 thin film

Abstract: We report a heterojunction formed between single-wall carbon nanotubes (SWCNTs) and a WO 3 thin film. WO 3 thin films were fabricated by sputter deposition of W followed by oxidation and SWCNTs were fabricated by the arc-discharge method. The morphology of the structures was examined by scanning electron microscopy, X-ray diffraction, and Raman spectroscopy. The current-voltage characteristics of WO 3 thin films, SWCNTs films, and SWCNT/WO 3 heterojunctions were measured in darkness and under ultraviolet light… Show more

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Cited by 14 publications
(9 citation statements)
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References 30 publications
(65 reference statements)
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“…55−58 The peak at around 927 cm −1 is attributed to the terminal −WO bonds, 57 25,55,57,58 The peak at the low wavenumber of 106 cm −1 comes from the lattice modes of crystalline WO 3 . 56 These characteristic peaks can be also found in the Raman spectrum of BGR−WO 3 NRs; besides, the typical D band (1346 cm −1 ) and G band (1597 cm −1 ) of graphene are detected, indicating the presence of both graphene and WO 3 . Compared to the spectrum of the bare WO 3 NRs, the peaks at 665, 757, and 814 cm −1 corresponding to the O−W−O vibration are broadened in the BGR−WO 3 NR Raman spectrum; in addition, the peak at 814 cm −1 is shifted to 806 cm −1 for the WO 3 in the BGR−WO 3 NR nanocomposites, probably due to the strong interaction between the WO 3 NRs and BGR, making the initial W−O bond weaker.…”
Section: Resultsmentioning
confidence: 70%
“…55−58 The peak at around 927 cm −1 is attributed to the terminal −WO bonds, 57 25,55,57,58 The peak at the low wavenumber of 106 cm −1 comes from the lattice modes of crystalline WO 3 . 56 These characteristic peaks can be also found in the Raman spectrum of BGR−WO 3 NRs; besides, the typical D band (1346 cm −1 ) and G band (1597 cm −1 ) of graphene are detected, indicating the presence of both graphene and WO 3 . Compared to the spectrum of the bare WO 3 NRs, the peaks at 665, 757, and 814 cm −1 corresponding to the O−W−O vibration are broadened in the BGR−WO 3 NR Raman spectrum; in addition, the peak at 814 cm −1 is shifted to 806 cm −1 for the WO 3 in the BGR−WO 3 NR nanocomposites, probably due to the strong interaction between the WO 3 NRs and BGR, making the initial W−O bond weaker.…”
Section: Resultsmentioning
confidence: 70%
“…We used 1000 ppm H 2 S gas diluted in nitrogen as the analyte gas. The gas was further diluted in dry air by varying the concentration of H 2 S gas at a constant dry air flow rate of 300 sccm when fed into the test chamber as previously reported 5 51 .…”
Section: Methodsmentioning
confidence: 99%
“…Synthesis was performed at an arc current density of 40 A/cm 2 in H 2 gas at 400 Torr for 4 min. The carbon source used was a graphite rod that contained catalyst wires of iron, nickel, and molybdenum 12 33 34 . The SWCNT template substrates were heat-treated at 400 °C in air for 2 h to remove amorphous carbon.…”
Section: Methodsmentioning
confidence: 99%