Composition formula of transparent conductive tin doped indium oxide in terms of cluster plus glue atom model

2020 ◽  
Vol 836 ◽  
pp. 155514
Author(s):  
Hao Liu ◽  
Yi Zhang ◽  
Xin Zhang ◽  
Quan Wang ◽  
Hualin Wang ◽  
...  
2011 ◽  
Vol 688 ◽  
pp. 395-399 ◽  
Author(s):  
Jian Bing Qiang ◽  
Liang Yuan ◽  
Qing Wang ◽  
Ying Min Wang ◽  
Chuang Dong ◽  
...  

With the aid of the atomic-cluster-plus-glue-atom model (ACPGA model) proposed by Dong et al [1] for bulk metallic glasses (BMGs), the formation and characteristic of Ni-Ta binary BMGs were investigated in this work. Binary glass-forming compositions containing 56.3–62.5 at.%-Ni were obtained by a composition formula [M-Ni6Ta6]Ni3based on the ACPGA model. It was found that Ni-Ta BMGs with a diameter of 2 mm was obtained over a composition range of 59 ~ 62 at.%-Ni by copper mold casting method, which are in good agreement with our model prediction. Newly-developed Ni–Ta BMGs are a kind of extreme materials, which exhibit superior thermal stability (Tg= 993K) and a ultrahigh fracture strength of about 3.5 GPa.


1988 ◽  
Vol 102 ◽  
pp. 215
Author(s):  
R.M. More ◽  
G.B. Zimmerman ◽  
Z. Zinamon

Autoionization and dielectronic attachment are usually omitted from rate equations for the non–LTE average–atom model, causing systematic errors in predicted ionization states and electronic populations for atoms in hot dense plasmas produced by laser irradiation of solid targets. We formulate a method by which dielectronic recombination can be included in average–atom calculations without conflict with the principle of detailed balance. The essential new feature in this extended average atom model is a treatment of strong correlations of electron populations induced by the dielectronic attachment process.


Author(s):  
I. A. Rauf

To understand the electronic conduction mechanism in Sn-doped indium oxide thin films, it is important to study the effect of dopant atoms on the neighbouring indium oxide lattice. Ideally Sn is a substitutional dopant at random indium sites. The difference in valence (Sn4+ replaces In3+) requires that an extra electron is donated to the lattice and thus contributes to the free carrier density. But since Sn is an adjacent member of the same row in the periodic table, the difference in the ionic radius (In3+: 0.218 nm; Sn4+: 0.205 nm) will introduce a strain in the indium oxide lattice. Free carrier electron waves will no longer see a perfect periodic lattice and will be scattered, resulting in the reduction of free carrier mobility, which will lower the electrical conductivity (an undesirable effect in most applications).One of the main objectives of the present investigation is to understand the effects of the strain (produced by difference in the ionic radius) on the microstructure of the indium oxide lattice when the doping level is increased to give high carrier densities. Sn-doped indium oxide thin films were prepared with four different concentrations: 9, 10, 11 and 12 mol. % of SnO2 in the starting material. All the samples were prepared at an oxygen partial pressure of 0.067 Pa and a substrate temperature of 250°C using an Edwards 306 coating unit with an electron gun attachment for heating the crucible. These deposition conditions have been found to give optimum electrical properties in Sn-doped indium oxide films. A JEOL 2000EX transmission electron microscope was used to investigate the specimen microstructure.


1988 ◽  
Vol 49 (C1) ◽  
pp. C1-215-C1-215
Author(s):  
R. M. MORE ◽  
G. B. ZIMMERMAN ◽  
Z. ZINAMON

2020 ◽  
Vol 190 (12) ◽  
pp. 1233-1260
Author(s):  
David K. Belashchenko

2007 ◽  
Vol 2007 (suppl_26) ◽  
pp. 489-494 ◽  
Author(s):  
J. Popović ◽  
E. Tkalčec ◽  
B. Gržeta ◽  
C. Goebbert ◽  
V. Ksenofontov ◽  
...  

2021 ◽  
Vol 133 ◽  
pp. 111078 ◽  
Author(s):  
Xing Liu ◽  
Lu Zhang ◽  
Yudong Li ◽  
Xianzhu Xu ◽  
Yunchen Du ◽  
...  

2020 ◽  
Vol 109 ◽  
pp. 101688
Author(s):  
Kazuhiko Yamada ◽  
Takumi Yamaguchi ◽  
Ryutaro Ohashi ◽  
Shinobu Ohki ◽  
Kenzo Deguchi ◽  
...  
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