Impact of Nanosize on Supercapacitance: Study of 1D Nanorods and

Mar 30, 2016 - B.C. Keswani , R.S. Devan , R.C. Kambale , A.R. James , S. Manandhar , Y.D. Kolekar , C.V. Ramana. Journal of Alloys and Compounds 2017...
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The impact of nanosize on supercapacitance: Study of 1D nanorods and 2D thin-film of nickel oxide Ranjit A. Patil, Cheng-Ping Chang, Rupesh S. Devan, Yung Liou, and Yuan-Ron Ma ACS Appl. Mater. Interfaces, Just Accepted Manuscript • Publication Date (Web): 30 Mar 2016 Downloaded from http://pubs.acs.org on March 30, 2016

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ACS Applied Materials & Interfaces

The impact of nanosize on supercapacitance: Study of 1D nanorods and 2D thin-films of nickel oxide Ranjit A. Patil,† Cheng-Ping Chang,† Rupesh S. Devan,† Yung Liou,‡ and Yuan-Ron Ma*,† †Department of Physics, National Dong Hwa University, Hualien 97401, Taiwan. ‡Institute of Physics, Academia Sinica, Taipei 11529, Taiwan.

ABSTRACT: We synthesized unique one-dimensional (1D) nanorods and two-dimensional (2D) thin-films of NiO on indium-tin-oxide thin films using hot-filament metal-oxide vapor deposition technique. The 1D nanorods have average width and length of ~100 nm and ~500 nm , and the densely-packed 2D thin-films have an average thickness of ~500 nm. The 1D nanorods perform as parallel units for charge storing. However, the 2D thin-films act as one single unit for charge storing. The 2D thin-films possess a high specific capacitance of ~746 F/g compared to 1D nanorods (~230 F/g) using galvanostatic charge-discharge measurements at a current density of 3 A/g. Since the 1D NiO nanorods provide plentiful surface areas than those of the 2D thinfilms, they are fully active at first few cycles. However the capacitance retention of the 1D nanorods decays faster than that of the 2D thin-films. Also, the 1D NiO nanorods suffer from instability due to the fast electrochemical dissolution and high nanocontact resistance. Electrochemical impedance spectroscopy verifies that, the low dimensionality of the 1D NiO nanorods induces the unavoidable effects that lead them to have poor supercapacitive

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performances. On the other hand, the slow electrochemical dissolution and small contact resistance in the 2D NiO thin-films favour to achieve high specific capacitance and great stability.

KEYWORDS 1D nanorod, 2D thin-film, nickel oxide, pseudocapacitance, nanocontact resistance, electrochemical impedance.



INTRODUCTION Electrochemical supercapacitors have been expansively explored as alternative energy storage

devices due to the power and energy densities larger than those of batteries, fuels cells and conventional

electrochemical

capacitors

with

characteristic

energy

storing.1,2

Since

supercapacitors possess high energy and power densities, they can be used in hybrid vehicles, industrial equipment, and other renewable energy storage.3,4 Abundantly, available carbon materials have provided high specific capacitance in the electrochemical double layer (EDL) mechanism, because of the large surface areas with porous surfaces and interlaced networks. However, carbon materials have limitations in the energy and power density due to the high contact resistances among the interlaced networks.5 The contact resistance therefore develops a high internal series resistance, and become a forerunner in poor performance.6 Also, carbon materials result in major time-dependent changes that deteriorate the charge storing response.7 Alternatively, pseudocapacitive materials, such as metal oxides and conducting polymers, can provide much high specific capacitance. However, conducting polymers suffer instability and fading in supercapacitor performance because of swelling and shrinking during the reduction and

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ACS Applied Materials & Interfaces

oxidation process.8 There are some other factors in exchange of ions/electrons, such as desirable morphology, crystallinity, and barrier-free accessibility, for controlling performance of electrochemical supercapacitor. To understand notion of charge storage mechanism in pseudocapacitive materials, efforts should be taken to improve the surface area, reduce resistive elements, and as small as possible barrier for the exchange of ions to attain high specific energy and power density. Transition metal oxides possess high specific energy and power density with excellent capacitance retention. Among transitional metal oxides, ruthenium oxide and ruthenium hydroxide show excellent capacitor performance,9-11 but they cost very high and are insufficient in deposit. Some metal oxides, such as MnO2,12 NiO,13-17 MoO2,18 and V2O5.19, are abundant and low-cost materials with similar capacitive performance. Nickel oxide and nickel hydroxide attract special interest due to the high theoretical capacitances values of 2584 F/g and 2082 F/g, respectively,20 which is much higher than that of MnO2 (1380 F/g).21 Moreover, NiO nanostructures have received plenty of attention due to several unique properties, such as low field-emission turn-on field (7.4 V/µm) with large current density (~160 µA/cm2),22 p-type semiconductor,23 wide bandgap (~3.7 eV),24 high (low) transparency of the bleached (colored) state,24 fast coloration and bleaching times (