scholarly journals Ion source design for industrial applications

Author(s):  
H. KAUFMAN ◽  
R. ROBINSON
2014 ◽  
Vol 85 (2) ◽  
pp. 02C306 ◽  
Author(s):  
N. Takahashi ◽  
H. Murata ◽  
H. Mitsubori ◽  
J. Sakuraba ◽  
T. Soga ◽  
...  

AIAA Journal ◽  
1982 ◽  
Vol 20 (6) ◽  
pp. 745-760 ◽  
Author(s):  
Harold R. Kaufman ◽  
Raymond S. Robinson

2017 ◽  
Vol 35 (4) ◽  
pp. 587-596 ◽  
Author(s):  
X.P. Zhu ◽  
L. Ding ◽  
Q. Zhang ◽  
Yu. Isakova ◽  
Y. Bondarenko ◽  
...  

AbstractHigh-intensity pulsed ion beam (HIPIB) technology is developed as an advanced manufacturing method for components with improved wear, corrosion and/or fatigue performance, etc. Robust HIPIB equipment with stable repetitive operation, long-lifetime, and easy maintenance are desired for industrial applications, on which stability of ion beam parameters is critical to achieve consistent result of reproducibility. Here, magnetically insulated ion diodes (MIDs) as ion source with durable graphite anode are investigated in a simple self-magnetic field configuration under repetitive operation. Influence of background pressure on ion beam generation and transportation is emphasized since ion beam sources were intrinsically a vacuum-based system. Comparative experiments were conducted on two types of HIPIB equipment, that is, TEMP-6 and TEMP-4M, differing in vacuum packages where turbo-molecular pump or oil diffusion pump was used. Both the HIPIB equipments are operated on a bipolar pulse mode, that is, a first negative pulse of 150–200 kV with pulse duration 450–500 ns to generate anode plasma on explosive electron emission, and a second positive pulse of 200–250 kV with 120 ns to accelerate the ions. Ion beam energy density up to 8 J/cm2 is achievable using MIDs of geometrical focusing configuration, and the total energy, energy density distribution along cross-section, deflection and divergence, and charge neutralization of the ion beams are assessed under background pressures in a wide range of two orders of magnitude, that is, 1–100 mPa. No appreciable change in the parameters is observed up to 50 mPa, and merely a slight increase in the beam deflection from about ±3 mm to about ±4 mm at the focal point over 50 mPa. The stability of ion beam at the varied pressure is mainly facilitated by the higher pressure up to several Pa in anode–cathode gap during plasma generation and good neutralizing effect for ion beam transportation.


2018 ◽  
Vol 25 (03) ◽  
pp. 1850066 ◽  
Author(s):  
Y. H. A. FAWZY ◽  
H. M. ABDEL-HAMID ◽  
M. M. EL-OKR ◽  
A. ATTA

Polyethylene terephthalate (PET) films with thickness 40[Formula: see text][Formula: see text]m are irradiated with 3[Formula: see text]keV argon ion beams with different fluence ranging from [Formula: see text][Formula: see text]ions.cm[Formula: see text] to [Formula: see text][Formula: see text]ions.cm[Formula: see text] using locally designed broad ion source. The changes in the PET structure are characterized using X-ray diffraction (XRD), Fourier transform infrared (FTIR) and scanning electron microscope (SEM) techniques. The XRD patterns show that the peak intensity decreases with irradiation and the particle size decreases from 65.75 Å for the un-irradiated to 52.80 Å after irradiation. The FTIR indicates partial decrease and reduction in the intensity of the bands due to the degradation of the polymer after ion irradiation. The optical energy band gap decreases from 3.14[Formula: see text]eV to 3.05[Formula: see text]eV and the number of carbon cluster increases from 119 to 126 after ion irradiation. The results show a slight increase in the electrical conductivities and the dielectric constant ([Formula: see text]). The results indicate the effectiveness of using PET films as capacitors and resistors in industrial applications.


2012 ◽  
Vol 83 (2) ◽  
pp. 02B914 ◽  
Author(s):  
Yong-Sub Cho ◽  
Dae-Il Kim ◽  
Han-Sung Kim ◽  
Kyung-Tae Seol ◽  
Hyeok-Jung Kwon ◽  
...  

Author(s):  
Dudley M. Sherman ◽  
Thos. E. Hutchinson

The in situ electron microscope technique has been shown to be a powerful method for investigating the nucleation and growth of thin films formed by vacuum vapor deposition. The nucleation and early stages of growth of metal deposits formed by ion beam sputter-deposition are now being studied by the in situ technique.A duoplasmatron ion source and lens assembly has been attached to one side of the universal chamber of an RCA EMU-4 microscope and a sputtering target inserted into the chamber from the opposite side. The material to be deposited, in disc form, is bonded to the end of an electrically isolated copper rod that has provisions for target water cooling. The ion beam is normal to the microscope electron beam and the target is placed adjacent to the electron beam above the specimen hot stage, as shown in Figure 1.


Author(s):  
C. F. Oster

Although ultra-thin sectioning techniques are widely used in the biological sciences, their applications are somewhat less popular but very useful in industrial applications. This presentation will review several specific applications where ultra-thin sectioning techniques have proven invaluable.The preparation of samples for sectioning usually involves embedding in an epoxy resin. Araldite 6005 Resin and Hardener are mixed so that the hardness of the embedding medium matches that of the sample to reduce any distortion of the sample during the sectioning process. No dehydration series are needed to prepare our usual samples for embedding, but some types require hardening and staining steps. The embedded samples are sectioned with either a prototype of a Porter-Blum Microtome or an LKB Ultrotome III. Both instruments are equipped with diamond knives.In the study of photographic film, the distribution of the developed silver particles through the layer is important to the image tone and/or scattering power. Also, the morphology of the developed silver is an important factor, and cross sections will show this structure.


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