Metal vapor vacuum-arc ion implantation effects on the adhesion and hardness of ion-beam deposited Cr/Cu films

2007 ◽  
Vol 253 (6) ◽  
pp. 3276-3283 ◽  
Author(s):  
Miao Yu ◽  
Jizhong Zhang ◽  
Dexing Li ◽  
Qingli Meng ◽  
Wenzhi Li
Keyword(s):  
Ion Implantation ◽  
Ion Beam ◽  
Metal Vapor ◽  
Vacuum Arc ◽  
Cu Films

Pattern Evolution of NiSi2 on Si Surface upon High Current Pulsed Ni Ion Implantation

2000 ◽  
Vol 648 ◽  
Author(s):  
X.Q. Cheng ◽  
H.N. Zhu ◽  
B.X. Liu
Keyword(s):  
Ion Implantation ◽  
Ion Beam ◽  
Fractal Dimensions ◽  
Metal Vapor ◽  
Ion Source ◽  
Vacuum Arc ◽  
High Current ◽  
Si Substrate ◽  
Kinetics Of ◽  
Si Wafer

AbstractFractal pattern evolution of NiSi2 grains on a Si surface was induced by high current pulsed Ni ion implantation into Si wafer using metal vapor vacuum arc ion source. The fractal dimension of the patterns was found to correlate with the temperature rise of the Si substrate caused by the implanting Ni ion beam. With increasing of the substrate temperature, the fractal dimensions were determined to increase from less than 1.64, to beyond the percolation threshold of 1.88, and eventually up to 2.0, corresponding to a uniform layer with fine NiSi2 grains. The growth kinetics of the observed surface fractals was also discussed in terms of a special launching mechanism of the pulsed Ni ion beam into the Si substrate.

Synthesis of Continuous SmSi2 Layers on Si by Samarium Ion Implantation Using A Metal Vapor Vacuum Arc Ion Source

2000 ◽  
Vol 647 ◽  
Author(s):  
X.Q. Cheng ◽  
H.N. Zhu ◽  
B.X. Liu
Keyword(s):  
Surface Morphology ◽  
Ion Implantation ◽  
Ion Beam ◽  
Metal Vapor ◽  
Ion Source ◽  
Vacuum Arc ◽  
Experimental Conditions ◽  
Post Annealing ◽  
Beam Heating ◽  
Fine Crystalline Structure

AbstractSamarium ion implantation was conducted to synthesize Sm-disilicide films on silicon wafers, using a metal vapor vacuum arc ion source and the continuous SmSi2 films were directly obtained with neither external heating during implantation nor post-annealing. Diffraction and surface morphology analysis confirmed the formed Sm-disilicilde films were of a fine crystalline structure under appropriate experimental conditions. Besides, the formation mechanism of the SmSi2phase is also discussed in terms of the temperature rise caused by ion beam heating and the effect of ion dose on the properties of the SmSi2films.

The influence of nanostructure formation on properties for Cr implanted PET

2001 ◽  
Vol 665 ◽  
Author(s):  
Wu Yuguang ◽  
Zhang Tonghe ◽  
Zhang Huixing ◽  
Zhang Xiaoji ◽  
Cui Ping ◽  
...  
Keyword(s):  
Wear Resistance ◽  
Ion Implantation ◽  
Metal Ion ◽  
Ion Beam ◽  
Dose Range ◽  
Surface Hardness ◽  
Metal Vapor ◽  
Vacuum Arc ◽  
Ion Beam Modification ◽  
Ion Implanted

ABSTRACTPolyethylene terephthalate (PET) has been modified by Cr ion implantation with a dose range from 1×1016to 2×1017ions /cm2 using a metal vapor vacuum arc MEVVA source. The surface morphology was observed by atomic force microscopy (AFM). The Cr atom precipitation was found. The changes of the structure and composition have been observed with transmission electron microscope (TEM). The TEM photos revealed the presence of Cr nano-meter particles on the implanted PET. It is believed that the change would cause the improvement of the conductive properties and wear resistance. The electrical properties of PET have been improved after metal ion implantation. The resistivity of Cr ion implanted PET decreased obviously with an increase of ion dose. When the metal ion dose with 2×1017cm−2 was implanted into PET, the resistivity of PET could be less than 0.1 Ωm. But when Si or C ions with same dose are implanted PET, the resistivity of PET would be up to several Ωm. The result show that the resistivity of Cr ion implanted sample is obviously lower than that of Si- and C-implanted one. After Cr implantation, the surface hardness and modulus could be increased. The property of the implanted PET has modified greatly. The hardness and modulus of Cr implanted PET with dose of 2×1017/cm2 is 9.5 and 3.1 times greater than that of pristine PET. So we can see that wear resistance improved greatly. The Cr ion beam modification mechanism of PET will be discussed.

THE VOID EFFECT OF MEVVA W ION IMPLANTATION ON THE TRIBOLOGICAL PROPERTIES OF H13 STEEL

2004 ◽  
Vol 11 (04n05) ◽  
pp. 363-366 ◽  
Author(s):  
JIANHUA YANG ◽  
TONGHE ZHANG
Keyword(s):  
Mechanical Properties ◽  
Ion Implantation ◽  
Ion Beam ◽  
Metal Vapor ◽  
Implantation Dose ◽  
Ion Source ◽  
Vacuum Arc ◽  
H13 Steel ◽  
Voltage Electron ◽  
Tungsten Concentration

H13 steel samples were implanted with tungsten using a metal vapor vacuum arc (MEVVA) ion source, with an implantation dose of 1×1017 cm -2, an extraction acceleration of 30 kV and pulsed ion beam fluxes of between 0.3 mA·cm -2 and 6 mA·cm -2. The surface mechanical properties and microstructure for the W-implanted samples was characterized by the Rutherford backscattering spectroscope (RBS) and a high voltage electron microscope (HVEM). Experimental results of wear and hardness indicated that the hardness and wear of H13 steel increased when the voids were produced by tungsten ion implantation with a high pulsed current density. Forming causes for voids and their influence on the tungsten concentration depth profile in the implanted H13 steel and the surface mechanical properties were discussed in terms of spike theory.

scholarly journals Formation of Buried Epitaxial Si-Ge Alloy Layers in Si Crystal by High Dose Ge ION Implantation

1991 ◽  
Vol 235 ◽  
Author(s):  
Kin Man Yu ◽  
Ian G. Brown ◽  
Seongil Im
Keyword(s):  
Ion Implantation ◽  
Single Crystal ◽  
Lattice Mismatch ◽  
Solid Phase ◽  
Metal Vapor ◽  
Ion Source ◽  
Vacuum Arc ◽  
High Dose ◽  
Solid Phase Epitaxy ◽  
Ion Channeling

ABSTRACTWe have synthesized single crystal Si1−xGex alloy layers in Si <100> crystals by high dose Ge ion implantation and solid phase epitaxy. The implantation was performed using the metal vapor vacuum arc (Mevva) ion source. Ge ions at mean energies of 70 and 100 keV and with doses ranging from 1×1016 to to 7×1016 ions/cm2 were implanted into Si <100> crystals at room temperature, resulting in the formation of Si1−xGex alloy layers with peak Ge concentrations of 4 to 13 atomic %. Epitaxial regrowth of the amorphous layers was initiated by thermal annealing at temperatures higher than 500°C. The solid phase epitaxy process, the crystal quality, microstructures, interface morphology and defect structures were characterized by ion channeling and transmission electron microscopy. Compositionally graded single crystal Si1−xGex layers with full width at half maximum ∼100nm were formed under a ∼30nm Si layer after annealing at 600°C for 15 min. A high density of defects was found in the layers as well as in the substrate Si just below the original amorphous/crystalline interface. The concentration of these defects was significantly reduced after annealing at 900°C. The kinetics of the regrowth process, the crystalline quality of the alloy layers, the annealing characteristics of the defects, and the strains due to the lattice mismatch between the alloy and the substrate are discussed.

Corrosion behavior of Zr modified CrN coatings using metal vapor vacuum arc ion implantation

2007 ◽  
Vol 25 (1) ◽  
pp. 110-116 ◽  
Author(s):  
K. P. Purushotham ◽  
L. P. Ward ◽  
N. Brack ◽  
P. J. Pigram ◽  
P. Evans ◽  
...  
Keyword(s):  
Ion Implantation ◽  
Corrosion Behavior ◽  
Metal Vapor ◽  
Vacuum Arc ◽  
Crn Coatings

Phase Transformation and Ion Beam Induced Crystallization in SiC Layers Formed by Mevva Implantation of Carbon into Silicon

1997 ◽  
Vol 481 ◽  
Author(s):  
Dihu Chen ◽  
S. P. Wong ◽  
L. C. Ho ◽  
H. Yan ◽  
R.W.M. Kwok
Keyword(s):  
Ion Beam ◽  
Strong Dependence ◽  
Metal Vapor ◽  
Ion Source ◽  
Vacuum Arc ◽  
Preparation Conditions ◽  
Random Nucleation ◽  
The One ◽  
Amorphous Sic ◽  
Induced Crystallization

ABSTRACTBuried SiC layers were synthesized by carbon implantation into silicon with a metal vapor vacuum arc ion source under various implantation and annealing conditions. The infrared absorption spectra of these samples were deconvoluted into two or three gaussian components depending on the preparation conditions. One component peaked at around 700 cm-1was assigned to amorphous SiC (a-SiC). The other two components, both peaked at 795 cm-1 but with different values of full width at half maximum (FWHM), were attributed to β-SiC. The one with a larger (smaller) FWHM corresponds to β-SiC of smaller (larger) grains. With this deconvolution scheme, the fraction of various SiC phases in these samples were determined. It was found that for the as-implanted samples there are critical energies and doses at which the crystalline SiC fraction increases abruptly. This was attributed to the ion beam induced crystallization (IBIC) effect. It was also shown that the IBIC effect leads to strong dependence of the β-SiC fraction on the order of implantation for samples synthesized by double-energy implantation. Analysis of the evolution of the β-SiC fraction with annealing time indicated that the crystallization process in these SiC layers could well be described by the classical random nucleation and growth theory.

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