The emission rates of CH, CD and C2spectral bands and a re-evaluation of the chemical sputtering yield of the JT-60U carbon divertor plates

2014 ◽  
Vol 54 (4) ◽  
pp. 043004 ◽  
Author(s):  
T. Nakano ◽  
S. Higashijima ◽  
H. Kubo ◽  
N. Asakura ◽  
M. Fukumoto
2002 ◽  
Vol 42 (6) ◽  
pp. 689-696 ◽  
Author(s):  
T. Nakano ◽  
H. Kubo ◽  
S. Higashijima ◽  
N. Asakura ◽  
H. Takenaga ◽  
...  

2001 ◽  
Vol T91 (1) ◽  
pp. 43 ◽  
Author(s):  
M. Zarrabian ◽  
A. Kallenbach ◽  
K. Behringer ◽  
A. Carlson ◽  
J. Gafert ◽  
...  

1999 ◽  
Vol T81 (1) ◽  
pp. 54 ◽  
Author(s):  
R. D. Monk ◽  
C. H. Amiss ◽  
H. Y. Guo ◽  
G. F. Matthews ◽  
G. M. McCracken ◽  
...  

2007 ◽  
Vol 1020 ◽  
Author(s):  
Gikan Takaoka ◽  
Masakazu Kawashita ◽  
Takeshi Okada

AbstractIn order to investigate the interactions of methanol cluster ion beams with solid surfaces, Si substrates and SiO2 films were irradiated at different acceleration voltages. The sputtered depth increased with increase of the acceleration voltage. When the acceleration voltage was 9 kV, the sputtered depths of Si and SiO2 at a dose of 1×1016ions/cm2 were 1497.1 nm and 147.8 nm, respectively. The selectivity between Si and SiO2 surfaces arose from the volatility of the reaction products. Furthermore, the sputtering yield for the Si surface was approximately seven hundreds times larger than that by Ar monomer ion beams. This suggested that chemical sputtering was predominant for the methanol cluster ion irradiation. In addition, the etching and cleaning process by the methanol cluster ion irradiation was performed on the Si surfaces contaminated with a small amount of metal particles such as Au and Al. Thus, methanol cluster ion beams have unique characteristics such as surface etching and cleaning with high sputtering yield and smooth surface.


2013 ◽  
Vol 833 ◽  
pp. 257-260
Author(s):  
Chuan Sun ◽  
Yun Kai Li ◽  
Hu Wang ◽  
Chang Chun Ge

in this work, two kinds of boron carbide coating based on copper substrates, which are non-FGM B4C/Cu coating and FGM B4C/Cu coating, have been fabricated successfully. It is found that the chemical sputtering yield of B4C measures by LAS2000 apparatus is much lower than that of SMF800 graphite under the conditions of 3keV, 4.6E 15D+ /s/cm2 irradiation, and that FGM-B4C coating has much better performance than non-FGM-B4C coating in thermal shock tests. Thermal desorption performance and physical sputtering damage after plasma irradiation are also evaluated.


2019 ◽  
Author(s):  
Chi-Yun Lin ◽  
Matthew Romei ◽  
Luke Oltrogge ◽  
Irimpan Mathews ◽  
Steven Boxer

Green fluorescent protein (GFPs) have become indispensable imaging and optogenetic tools. Their absorption and emission properties can be optimized for specific applications. Currently, no unified framework exists to comprehensively describe these photophysical properties, namely the absorption maxima, emission maxima, Stokes shifts, vibronic progressions, extinction coefficients, Stark tuning rates, and spontaneous emission rates, especially one that includes the effects of the protein environment. In this work, we study the correlations among these properties from systematically tuned GFP environmental mutants and chromophore variants. Correlation plots reveal monotonic trends, suggesting all these properties are governed by one underlying factor dependent on the chromophore's environment. By treating the anionic GFP chromophore as a mixed-valence compound existing as a superposition of two resonance forms, we argue that this underlying factor is defined as the difference in energy between the two forms, or the driving force, which is tuned by the environment. We then introduce a Marcus-Hush model with the bond length alternation vibrational mode, treating the GFP absorption band as an intervalence charge transfer band. This model explains all the observed strong correlations among photophysical properties; related subtopics are extensively discussed in Supporting Information. Finally, we demonstrate the model's predictive power by utilizing the additivity of the driving force. The model described here elucidates the role of the protein environment in modulating photophysical properties of the chromophore, providing insights and limitations for designing new GFPs with desired phenotypes. We argue this model should also be generally applicable to both biological and non-biological polymethine dyes.<br>


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