Deposition by pulsed erosion of nickel and aluminum on copper

Langner, J.; Piekoşzewski, J.; Pochrybniak, C.; Rosatelli, F.; Rizzo, Stefano; Kucinski, J.; Miotello, A.; Guzmàn, L.; Lazzeri, P.

doi:10.1016/0257-8972(94)90017-5

Cited by 9 publications

(3 citation statements)

References 7 publications

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“…Irradiation of solids with so-called plasma-ion beams is a strongly nonequilibrium process, which enables a number of effects that are impossible to achieve with other methods [2]. These include improvement of wettability of ceramics [3][4][5], production of stable copper-ceramics interfaces [6], production of stable Ni-Cu and Al-Cu interfaces [7], improvement of properties of zirconium alloys [8], improvement of tribological properties of stainless steel [9], improvement of high temperature oxidation resistance of stainless steel [10], modification of superconducting and electrical properties of Mg-B structures [11], improvement of manganese distribution in Si with He + and H + plasma pulse irradiation [12], doping metals with nitrogen [13], and photovoltaic junction formation [14].…”

Section: Introductionmentioning

confidence: 99%

Time evolution of the process of doping of solids by plasma-ion beams

Horodenski

Pochrybniak

2021

PPT

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Irradiation of a solid with intense plasma-ion beams produced within a high vacuumchamber (by the so-called Rod Plasma Injector [1]) is a strongly nonequilibrium process, which enablesachieving a number of effects which are impossible to be achieved with other methods. These are,amongst other: improvement of ceramics wettability, fabrication of stable copper-ceramics interfacesand stable Ni-Cu and Al-Cu interfaces, improvement of tribological properties and high temperatureoxidation resistance of stainless steel, photovoltaic junction formation, and many others. In the paper,the process of plasma-ion beam propagation regarding its time and energy distributions and the processof ion penetration of solids, resulting with ion implementation and temperature growth have beenanalyzed mathematically on basis of experimental data. Results of numerical calculations have beenpresented concerning temperature and dopant density time evolution.

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Section: Introductionmentioning

confidence: 99%

Time evolution of the process of doping of solids by plasma-ion beams

Horodenski

Pochrybniak

2021

PPT

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“…In the 90's, there appeared a great interest in the production of wear-resistant coating layers of TiN, TiC, and TiCN, on tools made of high-speed steel or sintered carbides [3,4,5]. Among different PID technologies, which have found wide applications in industrial practice, an important (and even predominant) role is played by plasma-arc techniques [2,3,5].…”

Section: Introductionmentioning

confidence: 99%

Application of arc-plasma discharges to coating of screw taps

et al. 2000

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The paper reports on results of technological research on the coating of standard screw taps with TiN layers deposited by means of arc-plasma discharges, which were carried out within a BULAT-type device equipped with three identical metal-plasma sources. Particular attention is paid to morphology of the coated surfaces. Some data about thickness and microhardness of the coating layers, as well as results of laboratory wear tests of the coated tools, are also presented.

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“…The production of fast ion beams has been studied since many decades [1], [2] in order to get a tool for surface treatment, like hardening, implementation and nano structering [3]- [7]. There are two kind of its production: direct static acceleration from a DC glow discharge or arc plasmas in a strong electric field and the indirect methode by generation inside of hot plasma.…”

Section: Introductionmentioning

confidence: 99%

KeV Ion Beam Generation from Z-Pinches Produced in Plasma Focus like Geometry

Engel¹,

Choi²,

Koshelev³

et al. 2000

Contrib. Plasma Phys.

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Dense Z-pinches produce strong soft X-ray and VUV emission with ns exposure when working with moderate current at the moment of maximum compression. Within these Z-pinches the Plasma focus geometry offers an efficient production of hot and dense plasmas (kT e more than 100 eV respectively N ion greater than 10 18 cm −3 ) in which also fast thermal ions are created. In order to design such a plasma focus of 1 m 3 laboratory size, which is equivalent to deliver a pinch current of around 200 kA, and a micro plasma focus, which gives 20 kA using a cm 3 scaled device, are investigated. Different direct and indirect diagnostic methods are presented in order to work out the required conditions for efficient ion beam production.

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Deposition by pulsed erosion of nickel and aluminum on copper

Cited by 9 publications

References 7 publications

Time evolution of the process of doping of solids by plasma-ion beams

Time evolution of the process of doping of solids by plasma-ion beams

Application of arc-plasma discharges to coating of screw taps

KeV Ion Beam Generation from Z-Pinches Produced in Plasma Focus like Geometry

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