foreign atom
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2020 ◽  
Vol 27 ◽  
pp. 115-121
Author(s):  
Evgenii Kalashnikov ◽  
Igor Tolstikhin ◽  
Nadezhda Belova

The discrete Frenkel-Kontorova model for the movement of a foreign atom in a solid, obtained in the local chains approximation, led to the movement of the atom in the Frenkel-Kontorova (F-K) soliton form. This model made it possible to reveal the structure of the F-K soliton, to design the shapes of nanostructures and to take into account their influence on the F-K soliton. The transition to field variables leads the Frenkel-Kontorova equation to the sine-Gordon equation for the displacement field of an atom having solutions also in the form of a soliton. This equation and its solution (soliton) contains coefficients depending on the shape and size of nanostructures. The transition to the sine-Gordon equation allowed us to use the results of Theodorakopoulos 's works related to the consideration of the interaction of elastic vibration modes with a soliton. This made it possible to calculate the diffusion coefficient of the soliton and find the dependence of the diffusion coefficient on the shape and size of nanostructures and temperature.


2019 ◽  
Vol 21 (20) ◽  
pp. 10587-10593 ◽  
Author(s):  
Si Zhou ◽  
Wei Pei ◽  
Qiuying Du ◽  
Jijun Zhao

Metal doped Au12 clusters have tunable catalytic activity for CO oxidation by M–Au bond order and d orbital center.


2018 ◽  
Vol 194 (1) ◽  
pp. 53-59
Author(s):  
Jyoti Thakur ◽  
Monika Tomar ◽  
Vinay Gupta ◽  
Manish K. Kashyap
Keyword(s):  

2018 ◽  
Vol 130 (31) ◽  
pp. 9923-9927 ◽  
Author(s):  
Yuanyuan Liu ◽  
Xiaoqi Chai ◽  
Xiao Cai ◽  
Mingyang Chen ◽  
Rongchao Jin ◽  
...  

2018 ◽  
Vol 57 (31) ◽  
pp. 9775-9779 ◽  
Author(s):  
Yuanyuan Liu ◽  
Xiaoqi Chai ◽  
Xiao Cai ◽  
Mingyang Chen ◽  
Rongchao Jin ◽  
...  

2015 ◽  
Vol 1802 ◽  
pp. 1-12
Author(s):  
Hiroshi Yao

ABSTRACTWe here present electronic structures and chiroptical responses of gold-based bimetallic nanoclusters protected by chiral thiolate ligand, glutathione (GSH), and compare them with those of monometallic counterparts. The nanoclusters examined are AuPd and AuAg bimetallic systems. The effect of Pd or Ag doping on the chiroptical responses of optically active Au nanoclusters as well as the importance of the bimetallic core configurations are discussed. Briefly, we find that GS-protected AuPd or AuAg nanoclusters exhibit quite different Cotton effects from those of the monometallic nanoclusters in metal-based electronic transition regions. In the AuPd system, all bimetallic nanoclusters exhibit featureless absorption profiles, but their circular dichroism (CD) signals are structured, offering a greater advantage in detecting a foreign atom doping in the nanocluster system. In the AuAg system, the nanocluster compounds exhibit relatively weaker CD responses than those of the corresponding Au compounds. This CD decrease can be explained in terms of the increased geometrical isomers that are formed by statistical distribution of Ag heteroatoms in the nanocluster, since an increased number of possible configurations gives an average in the CD response with positive and negative bands of different optical isomers.


2014 ◽  
Vol 2014 ◽  
pp. 1-7 ◽  
Author(s):  
Yanyan Gao ◽  
Xiaoping Zou ◽  
Zongbo Huang

Incorporated foreign atoms into the quantum dots (QDs) used in heterojunction have always been a challenge for solar energy conversion. A foreign atom indium atom was incorporated into PbS/CdS QDs to prepare In-PbS/In-CdS heterojunction by successive ionic layer adsorption and reaction method which is a chemical method. Experimental results indicate that PbS or CdS has been doped with In by SILAR method; the concentration of PbS and CdS which was doped In atoms has no significantly increase or decrease. In addition, incorporating of Indium atoms has resulted in the lattice distortions or changes of PbS or CdS and improved the light harvest of heterojunction. Using this heterojunction, Pt counter electrode and polysulfide electrolyte, to fabricate quantum dot sensitized solar cells, the short circuit current density ballooned to 27.01 mA/cm2from 13.61 mA/cm2and the open circuit voltage was improved to 0.43 V from 0.37 V at the same time.


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