Relaxation of charge imbalance in ad-wave superconductor

1996 ◽  
Vol 54 (5) ◽  
pp. 3044-3046 ◽  
Author(s):  
C. H. Choi
Keyword(s):  
Charge Imbalance

scholarly journals Further investigations into the effect of charge imbalance on luminescence production

2021 ◽  
pp. 118223
Author(s):  
M. Autzen ◽  
A.S. Murray ◽  
M. Jain ◽  
J.-P. Buylaert
Keyword(s):  
Charge Imbalance

scholarly journals Research on Molecular Structure and Electronic Properties of Ln3+ (Ce3+, Tb3+, Pr3+)/Li+ and Eu2+ Co-Doped Sr2Si5N8 via DFT Calculation

Molecules ◽  
2021 ◽  
Vol 26 (7) ◽  
pp. 1849
Author(s):  
Ziqian Yin ◽  
Meijuan Li ◽  
Jianwen Zhang ◽  
Qiang Shen
Keyword(s):  
Molecular Structure ◽  
Energy Level ◽  
Density Functional ◽  
Formation Energy ◽  
Electronic Band Structure ◽  
Blue Shift ◽  
Lanthanide Ions ◽  
Partial Replacement ◽  
Electronic Band ◽  
Charge Imbalance

We use density functional theory (DFT) to study the molecular structure and electronic band structure of Sr2Si5N8:Eu2+ doped with trivalent lanthanides (Ln3+ = Ce3+, Tb3+, Pr3+). Li+ was used as a charge compensator for the charge imbalance caused by the partial replacement of Sr2+ by Ln3+. The doping of Ln lanthanide atom causes the structure of Sr2Si5N8 lattice to shrink due to the smaller atomic radius of Ln3+ and Li+ compared to Sr2+. The doped structure’s formation energy indicates that the formation energy of Li+, which is used to compensate for the charge imbalance, is the lowest when the Sr2 site is doped. Thus, a suitable Li+ doping site for double-doped lanthanide ions can be provided. In Sr2Si5N8:Eu2+, the doped Ce3+ can occupy partly the site of Sr12+ ([SrN8]), while Eu2+ accounts for Sr12+ and Sr22+ ([SrN10]). When the Pr3+ ion is selected as the dopant in Sr2Si5N8:Eu2+, Pr3+ and Eu2+ would replace Sr22+ simultaneously. In this theoretical model, the replacement of Sr2+ by Tb3+ cannot exist reasonably. For the electronic structure, the energy level of Sr2Si5N8:Eu2+/Li+ doped with Ce3+ and Pr3+ appears at the bottom of the conduction band or in the forbidden band, which reduces the energy bandgap of Sr2Si5N8. We use DFT+U to adjust the lanthanide ion 4f energy level. The adjusted 4f-CBM of CeSr1LiSr1-Sr2Si5N8 is from 2.42 to 2.85 eV. The energy range of 4f-CBM in PrSr1LiSr1-Sr2Si5N8 is 2.75–2.99 eV and its peak is 2.90 eV; the addition of Ce3+ in EuSr1CeSr1LiSr1 made the 4f energy level of Eu2+ blue shift. The addition of Pr3+ in EuSr2PrSr2LiSr1 makes part of the Eu2+ 4f energy level blue shift. Eu2+ 4f energy level in EuSr2CeSr1LiSr1 is not in the forbidden band, so Eu2+ is not used as the emission center.

Estimating state-of-charge imbalance of batteries using force measurements

2016 ◽  
Author(s):  
Youngki Kim ◽  
Nassim A. Samad ◽  
Ki-Yong Oh ◽  
Jason B. Siegel ◽  
Bogdan I. Epureanu ◽  
...  
Keyword(s):  
State Of Charge ◽  
Force Measurements ◽  
Charge Imbalance

scholarly journals Stationary charge imbalance effect in a system of coupled Josephson junctions

2019 ◽  
Vol 127 (6) ◽  
pp. 67004
Author(s):  
K. V. Kulikov ◽  
M. Nashaat ◽  
Yu. M. Shukrinov
Keyword(s):  
Josephson Junctions ◽  
Charge Imbalance ◽  
Stationary Charge

scholarly journals Magnetic field and contact resistance dependence of non-local charge imbalance

2010 ◽  
Vol 21 (27) ◽  
pp. 274002 ◽  
Author(s):  
A Kleine ◽  
A Baumgartner ◽  
J Trbovic ◽  
D S Golubev ◽  
A D Zaikin ◽  
...  
Keyword(s):  
Magnetic Field ◽  
Contact Resistance ◽  
Charge Imbalance ◽  
Local Charge ◽  
Non Local
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