Electrochemical supercapacitor performance of SnO2 quantum dots
Graphical abstract
Introduction
Semiconductor quantum dots (QDs) plays vital role in technological and biological applications. However for an effective use of QDs, it is very important to understand their distinct physical and chemical properties with respect to their bulk counterparts. Wide band gap n-type semiconducting SnO2 nanostructures are well established for the use in technologically important applications like gas sensing, transparent electrodes, and as a catalyst [1], [2], [3], [4]. It is also found that the SnO2 is a potential material for much needed applications like solar cells [1], [5], [6], as anode materials in Li-ion battery [1], [7], [8], [9], [10], and electrochemical supercapacitors [11], [12], [13]. When compared with other metal oxides, SnO2 holds high electric conductivity (21.1 Ω.cm), high theoretical capacity, low potential of Li ion intercalation, as well as superior electron mobility (100–200 cm2/V.s). These properties made this material appealing for the energy storage applications [14], [15]. However, SnO2 or Sn-based anodes undergo a large volume changes of 200, 300% during the charging/discharging process for super capacitor and Li-ion battery applications, which leads to pulverization and loss of electrical contact between particles, subsequently, resulting in low capacity value and poor rate capability [16], [17], To overcome this problem, structures are inter-connected to compensate the volume change [18]. Alternatively, nano-sized crystals with dense stacking is used to reduce the volume variation [19], along with mixture structures are formed with other inactive substances, e.g., SnO2 with carbon [20], [21], in which the inactive carbon behave as a confining buffer for the volume variations. However these techniques could not solve the problem completely. Because of the in-active carbon, the total capacitance value reduces. Smaller size nanocrystals can provide good stability, an increased interface for the interaction between SnO2 and other species, leading to an enhanced performance in specific capacitance, power density [11], [16]. Cui et al. [11] reported pseudo capacitance of SnO2 QDs by adding 20% acetylene black, which they attributed to Faradic reactions between SnO2 QDs and the electrolyte. Shin et al. [22] reported maximum specific capacitance of 40.5 μF/cm2 and 8.9% loss of specific capacitance after 1000 cycles for the pure hierarchical SnO2 nanobranches without any carbon materials. SnO2 QDs exhibit a typical behavior in comparison with their bulk counterparts due to high surface to volume ratio and excitonic confinement effects [23], [24]. Thus, it is important to understand this distinct nature of QDs such that it can be used more effectively in applications. In the past, even though electrochemical studies were performed with the SnO2 QDs, however, the reason behind the better performance of the smaller size NPs is not well understood.
In the present work we have studied electrochemical super capacitor performance of the pure 2.4 and 25 nm nanoparticles (NPs) without adding any additives like carbon materials to observe the pure material behavior. These nanostructures are studied for their stoichiometry by using electron energy-loss spectroscopy (EELS), specific surface area by using Brunauer–Emmett–Teller (BET) method and aqua stability by studying the time dependent absorption spectra and Zeta potential measurements. Possible change in the volume of the NPs is probed by utilizing the temperature dependent Raman spectroscopy. Density functional theory (DFT) calculations are also carried out to calculate the charge distribution for each atom and the relaxed surface of the atoms. The stoichiometry, aqua stability, volume changes of these 2.4 and 25 nm NPs are compared for their electrochemical super capacitor performance.
Section snippets
Experimental section
SnO2 QDs were synthesized by soft chemical method. NH4OH (2 M) drops were added to aqueous SnCl4 (1 M) solution under continuous magnetic stirring at 80 °C. Precipitated white gel was washed with mille-pore water (18.2 MΩ.cm) several times to remove the Cl ions. The washed gel was dried at 100 °C and then crushed with a rotor. The as-prepared material was further annealed in air atmosphere using horizontal quartz tube furnace for 1 h at a temperature of 800 °C. Detailed synthesis process of NPs was
Results and discussion
Low magnification TEM image (Fig. 1a) shows spherical as-prepared SnO2 NPs. Average size of the as-prepared NPs (Fig. 1b) is around 2.4 nm, which is less than the Bohr radius of SnO2 (2.7 nm). HRTEM image in Fig. 1c manifests crystalline and spherical SnO2 QDs. Inset in Fig. 1c exhibits the zoomed image of single QD containing (110) crystalline plane of rutile tetragonal SnO2 phase (JCPDS #41-1445) with a d spacing of ∼ 0.345nm. The selective area electron diffraction (SAED) pattern of the QDs
Conclusion
SnO2 quantum dots (QDs) and bigger sized nanoparticles (NPs) of diameter 25 nm are studied as electrochemical super capacitor materials without adding any buffer materials. Dispersed QDs are found stable in water even after a month time. Electron energy-loss spectroscopic study of SnO2 QDs showed significant absence of stoichiometry. There is no apparent volume change in the QDs within the temperature range of 80 to 300 K. Excess of open volume in the non-stoichiometric QDs is made responsible
Acknowledgements
We acknowledge S. Amirthapandian, MPD, IGCAR for the EELS measurements and Dr. John Philip, SMARTS, IGCAR for the Zeta potential measurements.
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