scholarly journals Dual-cation preintercalated and amorphous carbon confined vanadium oxides as a superior cathode for aqueous zinc-ion batteries

Carbon ◽  
2022 ◽  
Vol 186 ◽  
pp. 160-170
Author(s):  
Xun Zhao ◽  
Lei Mao ◽  
Qihui Cheng ◽  
Fangfang Liao ◽  
Guiyuan Yang ◽  
...  
2019 ◽  
Vol 320 ◽  
pp. 134565 ◽  
Author(s):  
Wenbao Liu ◽  
Liubing Dong ◽  
Baozheng Jiang ◽  
Yongfeng Huang ◽  
Xianli Wang ◽  
...  

2020 ◽  
Vol 382 ◽  
pp. 122844 ◽  
Author(s):  
Hanmei Jiang ◽  
Yifu Zhang ◽  
Lei Xu ◽  
Zhanming Gao ◽  
Jiqi Zheng ◽  
...  

2021 ◽  
Vol 60 (4) ◽  
pp. 1517-1525
Author(s):  
Hongzhe Chen ◽  
Yao Rong ◽  
Zhanhong Yang ◽  
Lie Deng ◽  
Jian Wu

2021 ◽  
Author(s):  
Tao Zhou ◽  
Qing Han ◽  
Lingling Xie ◽  
Xinli Yang ◽  
Limin Zhu ◽  
...  

ChemNanoMat ◽  
2020 ◽  
Vol 6 (11) ◽  
pp. 1553-1566 ◽  
Author(s):  
Zhexuan Liu ◽  
Hemeng Sun ◽  
Liping Qin ◽  
Xinxin Cao ◽  
Jiang Zhou ◽  
...  

2021 ◽  
pp. 2111-2120
Author(s):  
Guoqun Zhang ◽  
Tao Wu ◽  
He Zhou ◽  
Hongrun Jin ◽  
Kaisi Liu ◽  
...  

Author(s):  
D. L. Misell

In the electron microscopy of biological sections the adverse effect of chromatic aberration on image resolution is well known. In this paper calculations are presented for the inelastic and elastic image intensities using a wave-optical formulation. Quantitative estimates of the deterioration in image resolution as a result of chromatic aberration are presented as an alternative to geometric calculations. The predominance of inelastic scattering in the unstained biological and polymeric materials is shown by the inelastic to elastic ratio, I/E, within an objective aperture of 0.005 rad for amorphous carbon of a thickness, t=50nm, typical of biological sections; E=200keV, I/E=16.


Author(s):  
H. Todokoro ◽  
S. Nomura ◽  
T. Komoda

It is interesting to observe polymers at atomic size resolution. Some works have been reported for thorium pyromellitate by using a STEM (1), or a CTEM (2,3). The results showed that this polymer forms a chain in which thorium atoms are arranged. However, the distance between adjacent thorium atoms varies over a wide range (0.4-1.3nm) according to the different authors.The present authors have also observed thorium pyromellitate specimens by means of a field emission STEM, described in reference 4. The specimen was prepared by placing a drop of thorium pyromellitate in 10-3 CH3OH solution onto an amorphous carbon film about 2nm thick. The dark field image is shown in Fig. 1A. Thorium atoms are clearly observed as regular atom rows having a spacing of 0.85nm. This lattice gradually deteriorated by successive observations. The image changed to granular structures, as shown in Fig. 1B, which was taken after four scanning frames.


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