Fabrication of nickel oxide-embedded titania nanotube array for redox capacitance application

2008 ◽  
Vol 53 (10) ◽  
pp. 3643-3649 ◽  
Author(s):  
Yibing Xie ◽  
Limin Zhou ◽  
Chuanjun Huang ◽  
Haitao Huang ◽  
Jian Lu
2009 ◽  
Vol 20 (7) ◽  
pp. 075502 ◽  
Author(s):  
Subarna Banerjee ◽  
Susanta K Mohapatra ◽  
Mano Misra ◽  
Indu B Mishra

2012 ◽  
Vol 1 (1) ◽  
pp. 39-44
Author(s):  
Hongyi Li ◽  
Jinshu Wang ◽  
Junshu Wu ◽  
Yucheng Du

2008 ◽  
Vol 37 (4) ◽  
pp. 416-417 ◽  
Author(s):  
Xiaomeng Wu ◽  
Yunhan Ling ◽  
Jianteng Sun ◽  
Xin Zhi ◽  
Zhaohui Huang

2010 ◽  
Vol 21 (38) ◽  
pp. 389801-389801 ◽  
Author(s):  
Maggie Paulose ◽  
Karthik Shankar ◽  
Oomman K Varghese ◽  
Gopal K Mor ◽  
Brian Hardin ◽  
...  

2004 ◽  
Vol 837 ◽  
Author(s):  
Maggie Paulose ◽  
Oomman K. Varghese ◽  
Karthik Shankar ◽  
Gopal K. Mor ◽  
Craig A. Grimes

ABSTRACTWe report on non-particulate titania photoelectrodes with a unique highly-ordered nanotube-array architecture prepared by an anodization process that enables precise control over array dimensions. Under 320–400 nm illumination titania nanotube-array photoanodes, pore size 110 nm, wall thickness 20 nm, and 6 μm length, generate hydrogen by water photoelectrolysis at a normalized rate of 80 mL/W•hr, to date the most efficient titania-based photoelectrochemical device, with a conversion efficiency of 12.25%. The highly-ordered nanotubular architecture allows for superior charge separation and charge transport, with a calculated quantum efficiency of nearly 100% for incident photons with energies larger than the titania bandgap.


2004 ◽  
Vol 835 ◽  
Author(s):  
Oomman K. Varghese ◽  
Gopal K. Mor ◽  
Maggie Paulose ◽  
Craig A. Grimes

ABSTRACTA tremendous variation in electrical resistance, from the semiconductor to metallic range, has been observed in titania nanotube arrays at room temperature, ≈25°C, in the presence of low ppm hydrogen gas concentrations (≤ 1000 ppm). The nanotube arrays are fabricated by anodizing titanium foil in an aqueous fluoride containing electrolyte solution. Subsequently, the arrays are annealed in an oxygen ambient, then coated with a 10 nm layer of palladium by evaporation. Electrical contacts are made by sputtering a small (e.g. 1 mm diameter) platinum disk atop the Pd coated nanotube-array. These sensors exhibit a resistance variation of the order of over 107 (1,000,000,000%) in the presence of 1000 ppm hydrogen at 23°C. To the best of our knowledge this dynamic change in electrical resistance the largest known response of any material, to any gas, at any temperature. The sensors demonstrate complete reversibility, repeatability, high selectivity, no drift and wide dynamic range. The nanoscale geometry of the nanotubes, in particular the points of tube-to-tube contact, is believed to be responsible for the outstanding hydrogen gas sensitivities.


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