scholarly journals Micro-Faraday cup matrix detector for ion beam measurements in fusion plasmas

2019 ◽  
Vol 90 (3) ◽  
pp. 033501
Author(s):  
D. I. Réfy ◽  
S. Zoletnik ◽  
D. Dunai ◽  
G. Anda ◽  
M. Lampert ◽  
...  
2004 ◽  
Vol 46 (2) ◽  
pp. 299-311 ◽  
Author(s):  
A. V. Melnikov ◽  
C. Hidalgo ◽  
A. A. Chmyga ◽  
N. B. Dreval ◽  
L. G. Eliseev ◽  
...  

MRS Bulletin ◽  
1988 ◽  
Vol 13 (12) ◽  
pp. 40-45 ◽  
Author(s):  
S.M. Rossnagel ◽  
J.J. Cuomo

Ion beam processing for thin film deposition is rapidly overtaking some of the more conventional plasma-based thin film processing techniques. This is due to strong improvements in the types and reliabilities of the sources available as well as a growing understanding of the advantages and capabilities of using ion beams.An ion beam process can be differentiated from a plasma-based process in that the plasma in an ion beam is generated away from the sample and a beam of ions is directed at the sample. In a plasma-based process, the sample is usually immersed in the plasma. This highlights the fundamental advantage of ion beam processing—control of the flux and energy of the ions incident on either a sample or a target (for sputter deposition). It is this control which is missing in plasma-based processing, where the ion flux (current), ion energy, chamber pressure, and gas species are all hopelessly intertwined. In addition, certain aspects of the ion bombardment—angle of incidence, complications of gas scattering, etc. —are essentially fixed in plasma-based processing, leaving no room to vary parameters, and in conjunction, film properties.A wealth of different types of ion sources cover a broad range of beam currents and energies. At the high energy end (0.1 – 20 MeV) are the implantation sources, typically used for doping semiconductors and treating surfaces (hardening, for example) and for various types of nuclear chemical analysis. These sources, however, tend to be very low current (μA). At slightly lower energies (tens of kilo-electron volts), but significantly higher currents (50 A), are the ion sources used for heating fusion plasmas.


2020 ◽  
Author(s):  
Yiren Li ◽  
Bin Miao ◽  
Xinjun Hao ◽  
Tielong Zhang ◽  
Yuming Wang

<p>For the calibration of space plasma analyzers, in particular low-energy ion mass spectrometers, a low energy ion beam system was developed. The positive ion beam is produced by a hot-cathode penning source and modified by a series of electrostatic lenses. And a 75 mm diameter 2-D imaging system and a Faraday cup mounted on movable arms are used for ion beam diagnostics. With protons as primary species, the system provides an ion beam in the energy range of 1 eV - 1000 eV with a large area ( ~ 50 cm<sup>2</sup>), highly parallel ( ± 0.5°), and spatially uniform ( ± 5%).</p>


2009 ◽  
Vol 80 (11) ◽  
pp. 113302 ◽  
Author(s):  
Lauri Panitzsch ◽  
Michael Stalder ◽  
Robert F. Wimmer-Schweingruber

2017 ◽  
Vol 24 (6) ◽  
pp. 063302 ◽  
Author(s):  
Vahid Damideh ◽  
Jalil Ali ◽  
Sor Heoh Saw ◽  
Rajdeep Singh Rawat ◽  
Paul Lee ◽  
...  

10.14311/396 ◽  
2003 ◽  
Vol 43 (1) ◽  
Author(s):  
M. Zoriy ◽  
F. Černý ◽  
D. Palamarchuk ◽  
S. Konvičková ◽  
I. Hüttel

Chromium nitride films are known as good protective layers for against both corrosion and wear. These coatings have been studied in detail during recent years. Their protective capability strongly depends on the deposition conditions. A modern method for preparing chromium nitride is the IBAD (Ion Beam Assisted Deposition) method. The main parameter determining the composition and properties of the films prepared by the IBAD method is the arrival ratio of impinging nitrogen ions to chromium atoms. In order to calibrate the ion beam XY-mechanical scanner with a Faraday cup, a detector was designed and constructed. By mathematical processing of the data, the flux of the nitrogen atoms was found. To obtain the flux of the chromium atoms the RBS and Talystep methods were used. Now, on the basis of this data, we can perform CrNx, coatings with controlled composition and properties.


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