Tritium-permeation-barrier properties of erbium oxide (TPB) coating on CLAM steel

2019 ◽  
Vol 138 ◽  
pp. 347-351 ◽  
Author(s):  
Shuai Liu ◽  
Xin Ju ◽  
Jie Qiu ◽  
Guoxiang Chen ◽  
Jun Sun ◽  
...  
2014 ◽  
Vol 89 (7-8) ◽  
pp. 1402-1405 ◽  
Author(s):  
Takumi Chikada ◽  
Masashi Shimada ◽  
Robert J. Pawelko ◽  
Takayuki Terai ◽  
Takeo Muroga

2011 ◽  
Vol 60 (1) ◽  
pp. 389-393 ◽  
Author(s):  
Takumi Chikada ◽  
Akihiro Suzuki ◽  
Hans Maier ◽  
Takayuki Terai ◽  
Takeo Muroga

2007 ◽  
Vol 367-370 ◽  
pp. 1033-1037 ◽  
Author(s):  
D. Levchuk ◽  
S. Levchuk ◽  
H. Maier ◽  
H. Bolt ◽  
A. Suzuki

2009 ◽  
Vol 56 (1) ◽  
pp. 309-313 ◽  
Author(s):  
Takumi Chikada ◽  
Akihiro Suzuki ◽  
Tomohiro Kobayashi ◽  
Zhenyu Yao ◽  
Denis Levchuk ◽  
...  

2021 ◽  
Author(s):  
Lu Wang ◽  
Hai-Shan Zhou ◽  
Hao-Dong Liu ◽  
Yu-Ping Xu ◽  
Wan-Jing Wang ◽  
...  

Abstract Tritium (T) permeation through plasma-facing component (PFC) into the coolant is a major concern of fusion reactor operation. In this work, deuterium (D) permeation through CLAM steel, CLAM/CLAM and CLAM/Fe-Cr-Al samples prepared by hot isostatic pressing (HIP) are tested in a linear plasma device. Only the downstream surfaces of the samples are oxidized with controlled atmosphere to form permeation barrier. No significant effect on D diffusion and penetration can be observed for the joining interfaces, while the dense oxide layer at the downstream side plays an important role in suppressing D permeation. The downstream surface oxidization of CLAM/Fe-Cr-Al is found to effectively reduce D permeation flux by a factor up to 1000.


2010 ◽  
Vol 85 (7-9) ◽  
pp. 1401-1405 ◽  
Author(s):  
Shuai Liu ◽  
Xin Ju ◽  
Yong Xin ◽  
Jie Qiu ◽  
Tao Li ◽  
...  

Author(s):  
B. Van Deurs ◽  
J. K. Koehler

The choroid plexus epithelium constitutes a blood-cerebrospinal fluid (CSF) barrier, and is involved in regulation of the special composition of the CSF. The epithelium is provided with an ouabain-sensitive Na/K-pump located at the apical surface, actively pumping ions into the CSF. The choroid plexus epithelium has been described as “leaky” with a low transepithelial resistance, and a passive transepithelial flux following a paracellular route (intercellular spaces and cell junctions) also takes place. The present report describes the structural basis for these “barrier” properties of the choroid plexus epithelium as revealed by freeze fracture.Choroid plexus from the lateral, third and fourth ventricles of rats were used. The tissue was fixed in glutaraldehyde and stored in 30% glycerol. Freezing was performed either in liquid nitrogen-cooled Freon 22, or directly in a mixture of liquid and solid nitrogen prepared in a special vacuum chamber. The latter method was always used, and considered necessary, when preparations of complementary (double) replicas were made.


Author(s):  
E. I. Alessandrini ◽  
M. O. Aboelfotoh

Considerable interest has been generated in solid state reactions between thin films of near noble metals and silicon. These metals deposited on Si form numerous stable chemical compounds at low temperatures and have found applications as Schottky barrier contacts to silicon in VLSI devices. Since the very first phase that nucleates in contact with Si determines the barrier properties, the purpose of our study was to investigate the silicide formation of the near noble metals, Pd and Pt, at very thin thickness of the metal films on amorphous silicon.Films of Pd and Pt in the thickness range of 0.5nm to 20nm were made by room temperature evaporation on 40nm thick amorphous Si films, which were first deposited on 30nm thick amorphous Si3N4 membranes in a window configuration. The deposition rate was 0.1 to 0.5nm/sec and the pressure during deposition was 3 x 10 -7 Torr. The samples were annealed at temperatures in the range from 200° to 650°C in a furnace with helium purified by hot (950°C) Ti particles. Transmission electron microscopy and diffraction techniques were used to evaluate changes in structure and morphology of the phases formed as a function of metal thickness and annealing temperature.


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