Secondary battery technologies: a static potential for power

Author(s):  
Pavlos Nikolaidis ◽  
Andreas Poullikkas
Author(s):  
H. Kohl

High-Resolution Electron Microscopy is able to determine structures of crystals and interfaces with a spatial resolution of somewhat less than 2 Å. As the image is strongly dependent on instrumental parameters, notably the defocus and the spherical aberration, the interpretation of micrographs necessitates a comparison with calculated images. Whereas one has often been content with a qualitative comparison of theory with experiment in the past, one is currently striving for quantitative procedures to extract information from the images [1,2]. For the calculations one starts by assuming a static potential, thus neglecting inelastic scattering processes.We shall confine the discussion to periodic specimens. All electrons, which have only been elastically scattered, are confined to very few directions, the Bragg spots. In-elastically scattered electrons, however, can be found in any direction. Therefore the influence of inelastic processes on the elastically (= Bragg) scattered electrons can be described as an attenuation [3]. For the calculation of high-resolution images this procedure would be correct only if we had an imaging energy filter capable of removing all phonon-scattered electrons. This is not realizable in practice. We are therefore forced to include the contribution of the phonon-scattered electrons.


1998 ◽  
Vol 70 (1) ◽  
pp. 170
Author(s):  
Y Idota
Keyword(s):  

2021 ◽  
Vol 33 (10) ◽  
pp. 2004902
Author(s):  
Myeong Hwan Lee ◽  
Jongha Lee ◽  
Sung‐Kyun Jung ◽  
Dayoung Kang ◽  
Myung Soo Park ◽  
...  

2020 ◽  
Vol 2020 (9) ◽  
Author(s):  
Cesar Ayala ◽  
Xabier Lobregat ◽  
Antonio Pineda

Abstract We give the hyperasymptotic expansion of the energy of a static quark-antiquark pair with a precision that includes the effects of the subleading renormalon. The terminants associated to the first and second renormalon are incorporated in the analysis when necessary. In particular, we determine the normalization of the leading renormalon of the force and, consequently, of the subleading renormalon of the static potential. We obtain $$ {Z}_3^F $$ Z 3 F (nf = 3) = $$ 2{Z}_3^V $$ 2 Z 3 V (nf = 3) = 0.37(17). The precision we reach in strict perturbation theory is next-to-next-to-next-to-leading logarithmic resummed order both for the static potential and for the force. We find that the resummation of large logarithms and the inclusion of the leading terminants associated to the renormalons are compulsory to get accurate determinations of $$ {\Lambda}_{\overline{\mathrm{MS}}} $$ Λ MS ¯ when fitting to short-distance lattice data of the static energy. We obtain $$ {\Lambda}_{\overline{\mathrm{MS}}}^{\left({n}_f=3\right)} $$ Λ MS ¯ n f = 3 = 338(12) MeV and α(Mz) = 0.1181(9). We have also MS found strong consistency checks that the ultrasoft correction to the static energy can be computed at weak coupling in the energy range we have studied.


2019 ◽  
Vol 7 (47) ◽  
pp. 27057-27065 ◽  
Author(s):  
Jinkwang Hwang ◽  
Koki Takeuchi ◽  
Kazuhiko Matsumoto ◽  
Rika Hagiwara

NaV2(PO4)3 is prepared by chemical desodiation of Na3V2(PO4)3 using Cl2 gas, and the mixture of Na3V2(PO4)3 and NaV2(PO4)3 is used as a novel and reliable NASICON-type counter electrode for Na secondary battery tests.


1990 ◽  
pp. 1-11 ◽  
Author(s):  
Tsutomu MATSUNAGA ◽  
Hideharu DAIFUKU ◽  
Takahiro KAWAGOE

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