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Online since: August 2013
Authors: Dian Wu Huang, Dan Liu, Ru Chen, Li Xia Yuan
It could be seen that all these XRD peaks could be indexed as the hexagonal ZnO, consistent with the values in the standard card (JCPDS 36-1451).
The growth units of the ZnO crystals are the complex of in the hydrothermal process, whose coordination numbers of Zn2+ is four.
The growth units of the ZnO crystals are the complex of in the hydrothermal process, whose coordination numbers of Zn2+ is four.
Online since: August 2019
Authors: Chi Hoon Kim, Vaibhav Lokhande, Taek Soo Ji
Next, the pseudocapacitor stores energy by using a change in the number of atoms of the metal existing in the metal oxide of the electrode material or a reduction/oxidation reaction of the conductive polymer (polypyrrole, polyaniline, etc.) [3].
The peaks at angle 2θ of 14.1, 23.10, 24.3, 27.1 and 28.2 correspond to (100), (001), (110), (101) and (200) respectively and are indexed to the hexagonal phase of WO3 (JCPDS card no. 00-0033-1387).
The peaks at angle 2θ of 14.1, 23.10, 24.3, 27.1 and 28.2 correspond to (100), (001), (110), (101) and (200) respectively and are indexed to the hexagonal phase of WO3 (JCPDS card no. 00-0033-1387).
Online since: September 2013
Authors: Yan Zhao, Dao Jiang Gao, Guang Liang Xu, Chun Yan Wu, Dan Qin, Xin Lai, Si Wu, Hong Feng, Tao Li, Jian Bi
The XRD pattern of the obtained SrWO4 microcrystallines in Fig. 1A-C shows that all the peaks can be indexed as a pure tetragonal scheelite structure (JCPDS card 85-0587) and no other impurities were observed in the products, which confirms that the as-prepared products are SrWO4.
At the present stage, a number of OH- ions selectively adsorbed on different crystallographic planes.
At the present stage, a number of OH- ions selectively adsorbed on different crystallographic planes.
Online since: October 2007
Authors: Han Zhou, Tong Xiang Fan, Di Zhang
Consequently, to prepare hollow spheres cocci is a good
candidate as biotemplates for encapsulation which offers some distinct advantages: firstly, since the
abundant functional groups on the cell walls are inherited from the bacteria which are able to bind
metal cations or polar molecules through coordination or electrostatic interactions, no surface
modification or activation steps are required, which reduces the number of processing steps and saves
time.
The XRD pattern of bacteria/ZnO core-shell spheres without calcination in Fig. 1a is similar with that of calcined at 700˚C in Fig. 1b except for lower intensity of the diffraction peaks, comfirming that the shells of the two samples are composed of wurtzite ZnO (JCPDS card NO. 36-1451, a=3.249Å, c=5.206Å) nanocrystals.
The XRD pattern of bacteria/ZnO core-shell spheres without calcination in Fig. 1a is similar with that of calcined at 700˚C in Fig. 1b except for lower intensity of the diffraction peaks, comfirming that the shells of the two samples are composed of wurtzite ZnO (JCPDS card NO. 36-1451, a=3.249Å, c=5.206Å) nanocrystals.
Online since: November 2010
Authors: Shi Xi Yu, Guo En Luo, Ying Luo, Wei Liu, Xiao Yuan Yu
All the patterns can be indexed to a single-phase material having an orthorhombic olivine-type structure with space group of Pnma, which is corresponded to the reference LiFePO4 spectrum (JCPDS card NO. 83-2029).
And the LiFePO4/C contained 7%wt PS showed the best electrochemical performance Fig. 4 discharge capacity versus cycle numbers of LiFePO4 cell at 0.1C rate between 2.5 and 4.1V The cyclic voltammetry curves of LiFePO4/C electrodes with different carbon content were shown in Fig.5.
And the LiFePO4/C contained 7%wt PS showed the best electrochemical performance Fig. 4 discharge capacity versus cycle numbers of LiFePO4 cell at 0.1C rate between 2.5 and 4.1V The cyclic voltammetry curves of LiFePO4/C electrodes with different carbon content were shown in Fig.5.
Online since: January 2013
Authors: Xue Feng Bai, Wei Wu
As shown in Fig. 1A, all the diffraction peaks could be well indexed to pure hexagonal phase of ZnIn2S4 (ICSD-JCPDS card No. 01-072-0773).
When the impure ion concentration was low-level, the number of the trapping sites was increased; however, when the impure ion concentration was excessive, the abundant trapping sites as recombination centers could make charge carriers inactive due to be trapped several times.
When the impure ion concentration was low-level, the number of the trapping sites was increased; however, when the impure ion concentration was excessive, the abundant trapping sites as recombination centers could make charge carriers inactive due to be trapped several times.
Online since: March 2013
Authors: Li Zhen Yang, Qiang Chen, Yue Fei Zhang, Yong He Li, Yu Jie Li, Hao Yu Fu
A number of approaches have been developed to fabricate various structural and morphological Ag/C nanocables[6-10].
All strong peaks marked with black arrows can be indexed to the diffraction of (111), (200), (220) and (311) planes of face-centered cubic (fcc) silver [space group: Fm3m (225)], which really coincided with (JCPDS Card No. 04-0783).
All strong peaks marked with black arrows can be indexed to the diffraction of (111), (200), (220) and (311) planes of face-centered cubic (fcc) silver [space group: Fm3m (225)], which really coincided with (JCPDS Card No. 04-0783).
Online since: June 2014
Authors: P. Devendran, T. Alagesan, K. Pandian
The C-H bending vibration comes around at 847 cm-1and also the corresponding intensity of Bi-S bond (PVA-Bi2S3@CS) are decreased for the reason that the size of Bi2S3 NRs converted into very small size, so easily adsorbed on CSs as shown in Fig.1(d).
3.2 Structural and Morphological Studies
The positions and relative intensities of all the peaks are in good conformity with those of the orthorhombic crystal structure of Bi2S3 and are indexed according to JCPDS card number 17-0320.The broadening of the peaks clearly indicates that the size of the product is in
Fig. 2: XRD spectrum of Bi2S3 NRs coated on carbon spheres, (a) - without PVP, (b) - low Concentration of PVP, (c) - high concentration of PVP.
Online since: January 2013
Authors: Shu Guang Chen, Hai Bin Li, Yan De Song
The peaks at 2θ = 32.5°, 35.5°, 38.7°, 48.7°, 53.4°, 58.3°, 61.5°, 65.8°, 66.24°, 67.9° can be perfectly indexed to the characteristic diffractions of CuO monoclinic phase (JCPDS Card No. 45-0937).
As shown in Fig. 3a, a large number of CuO nanosheets with high dispersity can be clearly seen in the picture.
As shown in Fig. 3a, a large number of CuO nanosheets with high dispersity can be clearly seen in the picture.