Experimental study of single vs. two-close-frequency heating impact on confinement and losses dynamics in ECR Ion Sources plasmas by means of X-ray spectroscopy and imaging

Author(s):  
David Mascali ◽  
Eugenia Naselli ◽  
Richard Racz ◽  
Sándor Biri ◽  
Luigi Celona ◽  
...  

Abstract We hereby report the study of confinement and electron losses dynamics in the magnetic trap of an Electron Cyclotron Resonance Ion Source (ECRIS) using a special multi-diagnostic setup that has allowed the simultaneous collection of plasma radio-self-emission and X-ray images in the range 500 eV - 20 keV. Argon plasmas were generated in single and two close frequency heating (TCFH) modes. Evidences of turbulent regimes have been found: for stable and unstable configurations quantitative characterizations of the plasma radio self-emission have been carried out, then compared with local measurement of plasma energy content evaluated by X-ray imaging. This imaging method is the only one able to clearly separate X-ray radiation coming from the plasma from the one coming from the plasma chamber walls. X-ray imaging has been also supported and benchmarked by volumetric spectroscopy performed via SDD and HPGe detectors. The obtained results in terms of X-ray intensity signal coming from the plasma core and from the plasma chamber walls have permitted to estimate the average ratio: plasma vs. walls (i.e., plasma losses) as a function of input RF power and pumping wave frequency, showing an evident increase (above the experimental errors) of the intensity in the 2-20 keV energy range due to the plasma losses in case of unstable plasma. This ratio was well correlated with the strength of the instabilities, in single frequency heating (SFH) operation mode; in TCFH mode, under specific power balance conditions and frequency combinations, it was possible to damp the instabilities, thus the plasma losses were observed to decrease and a general reconfiguration of the spatial plasma structure occurred (the X-ray emission was more concentrated in the center of the plasma chamber). In the end, a simplified model has been used to simulate electron heating under different pumping frequencies, discussing the impact of velocity anisotropy vs. the onset of the instability, and the mechanism of particles diffusion in the velocity space in stable and unstable regimes.

2007 ◽  
Vol 204 (8) ◽  
pp. 2734-2739 ◽  
Author(s):  
K. Mizuno ◽  
Y. Furuya ◽  
K. Hirano ◽  
H. Okamoto

2021 ◽  
Vol 16 (08) ◽  
pp. P08037
Author(s):  
C.H. Lim ◽  
J. Lee ◽  
Y. Choi ◽  
J.W. Park ◽  
H.K. Kim

2014 ◽  
Vol 87 (7) ◽  
pp. 278-283
Author(s):  
Naoya AMINO ◽  
Yasuhiro ISHIKAWA ◽  
Masaki SATO
Keyword(s):  
X Ray ◽  

2014 ◽  
Vol 752 ◽  
pp. 485-496 ◽  
Author(s):  
G. Agbaglah ◽  
R. D. Deegan

AbstractWe study the formation, growth and disintegration of jets following the impact of a drop on a thin film of the same liquid for $\def \xmlpi #1{}\def \mathsfbi #1{\boldsymbol {\mathsf {#1}}}\let \le =\leqslant \let \leq =\leqslant \let \ge =\geqslant \let \geq =\geqslant \def \Pr {\mathit {Pr}}\def \Fr {\mathit {Fr}}\def \Rey {\mathit {Re}}\mathit{We}<1000$ and $\mathit{Re}<2000$ using a combination of numerical simulations and linear stability theory (Agbaglah, Josserand & Zaleski, Phys. Fluids, vol. 25, 2013, 022103). Our simulations faithfully capture this phenomena and are in good agreement with experimental profiles obtained from high-speed X-ray imaging. We obtain scaling relations from our simulations and use these as inputs to our stability analysis. The resulting predictions for the most unstable wavelength are in excellent agreement with experimental data. Our calculations show that the dominant destabilizing mechanism is a competition between capillarity and inertia but that deceleration of the rim provides an additional boost to growth. We also predict over the entire parameter range of our study the number and timescale for formation of secondary droplets formed during a splash, based on the assumption that the most unstable mode sets the droplet number.


2017 ◽  
Vol 7 ◽  
pp. 1634-1636 ◽  
Author(s):  
V. Koukou ◽  
N. Martini ◽  
G. Fountos ◽  
C. Michail ◽  
A. Bakas ◽  
...  

2011 ◽  
Vol 690 ◽  
pp. 5-15 ◽  
Author(s):  
L. V. Zhang ◽  
J. Toole ◽  
K. Fezzaa ◽  
R. D. Deegan

AbstractWe used optical and X-ray imaging to observe the formation of jets from the impact of a single drop with a deep layer of the same liquid. For high Reynolds number there are two distinct jets: the thin, fast and early-emerging ejecta; and the slow, thick and late-emerging lamella. For low Reynolds number the two jets merge into a single continuous jet, the structure of which is determined by the distinct contributions of the lamella and the ejecta. We measured the emergence time, position and speed of the ejecta sheet, and find that these scale as power laws with the impact speed and the viscosity. We identified the origin of secondary droplets with the breakup of the lamella and the ejecta jets, and show that the size of the droplets is not a good indicator of their origin.


2018 ◽  
Vol 45 (4) ◽  
pp. 175-182
Author(s):  
Yuji Sato

Appearance of bubbles in the rubber has been observed in real time by using X-ray imaging method in SPring-8. The behavior of diameter and quantity of bubbles has been measured for the samples which have the various contents of cure agent and moisture. The babbles appear after 30 to 50 sec from releasing curing pressure at the place where there are no any feature in the X-ray images pixel size is 0.5 μm. The diameter of bubbles increases linearly with time at first, and then it grows up to be closer to the limit diameter finally. This final diameter changes with cure time and amount of cure agent. And the quantity of bubbles changes with amount of moisture. The result shows the one of origin of bubbles is moisture, and even if the moisture content changes, the size of moisture particles does not change, the quantity of particles changes. The crosslink density participates in whether this particle changes to a bubble or keeps that state. That also participates in the final diameter of bubble. X-Ray experiments were performed at BL19B2, BL46XU in the SPring-8 with approval of the Japan Radiation Research Institute (JASRI) Proposal No. 2014A1571,2014A1572).


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