2017
DOI: 10.3390/coatings7110185
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Surface Texturing of CVD Diamond Assisted by Ultrashort Laser Pulses

Abstract: Diamond is a wide bandgap semiconductor with excellent physical properties which allow it to operate under extreme conditions. However, the technological use of diamond was mostly conceived for the fabrication of ultraviolet, ionizing radiation and nuclear detectors, of electron emitters, and of power electronic devices. The use of nanosecond pulse excimer lasers enabled the microstructuring of diamond surfaces, and refined techniques such as controlled ablation through graphitization and etching by two-photon… Show more

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Cited by 46 publications
(34 citation statements)
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References 92 publications
(119 reference statements)
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“…CVD is another method of deposition under vacuum and is the process of chemically reacting a volatile compound from a material to be deposited with other gases, in order to produce a non-volatile thermal properties-this means that one can combine deposition methods, like layers of PVD and CVD, in the same coating [23][24][25][26].…”
Section: Introductionmentioning
confidence: 99%
“…CVD is another method of deposition under vacuum and is the process of chemically reacting a volatile compound from a material to be deposited with other gases, in order to produce a non-volatile thermal properties-this means that one can combine deposition methods, like layers of PVD and CVD, in the same coating [23][24][25][26].…”
Section: Introductionmentioning
confidence: 99%
“…The existence of HSFL allows for the generation of much smaller periods Λ down to ~λ/4–λ/5 in the case of diamond 30 32 . Indeed, HSFL with periodicities down to ~λ/8 can be found when graphitic-like phases are generated 33 .…”
Section: Introductionmentioning
confidence: 99%
“…The periodical ripples or laser-induced periodic surface structure (LIPSS) derive from the interference of the incident laser with quasi-monochromatic plasmons or among themselves. In this regime, the produced periodicity of LIPSS, approximately λ/4, is much smaller than λ [27], and can be calculated as Λ = λ/2n = 167 nm for normal incidence, where λ = 800 nm is the wavelength of the fs laser applied in this work and n = 2.40 is the real part of the complex refractive index of diamond [28]. The orientation of the LIPSS is perpendicular to the laser polarization direction.…”
Section: Influence Of Effective Number Of Pulses On Cvd Diamond Coatimentioning
confidence: 95%