2011
DOI: 10.1063/1.3569763
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Formation of subwavelength grating on molybdenum mirrors using a femtosecond Ti:sapphire laser system operating at 10 Hz

Abstract: We report formation of subwavelength surface grating over large surface area of molybdenum mirror by multiple irradiation of amplified femtosecond laser pulses from a homemade Ti:sapphire oscillator-amplifier laser system in a raster scan configuration. The laser system delivered 2 mJ, 80 fs duration laser pulses at a pulse repetition rate of 10 Hz. Various parameters such as pulse fluence, number of pulses, laser polarization, scan speed, and scan steps were optimized to obtain uniform subwavelength gratings.… Show more

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Cited by 8 publications
(3 citation statements)
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“…For example, it was observed that the spacing of FLIPSS produced on platinum at a laser fluence of 0.084J/cm 2 decreased from 0.62 to 0.55 μm with an increase in the number of laser shots from 30 to 500 due to modification of the FLIPSS morphology. This effect was also studied in (Mo), (NiTi alloy), (CuZn alloy, ZnO, diamond), and (Si). The effect of the laser fluence on the FLIPSS period was studied in .…”
Section: Femtosecond Laser‐induced Periodic Structures On Metalsmentioning
confidence: 99%
“…For example, it was observed that the spacing of FLIPSS produced on platinum at a laser fluence of 0.084J/cm 2 decreased from 0.62 to 0.55 μm with an increase in the number of laser shots from 30 to 500 due to modification of the FLIPSS morphology. This effect was also studied in (Mo), (NiTi alloy), (CuZn alloy, ZnO, diamond), and (Si). The effect of the laser fluence on the FLIPSS period was studied in .…”
Section: Femtosecond Laser‐induced Periodic Structures On Metalsmentioning
confidence: 99%
“…A mechanically polished Mo plate with a purity of 99.98% was selected as the sample because of its high elasticity modulus and its thermal and electrical conductivity properties, which are useful for wide applications in microelectronics, photoelectronics, laser and space optics, and fusion reactors. , The experiments were implemented with a line-scanning method through the precise translation of the sample via a computer-controlled X-Y-Z stage (Newport, UTM100 PPE1). The focal laser spot on the sample surface, which was placed at a position 400 mm away from the focus to avoid air ionization disturbance, was measured as 2ω 0 = 80 μm (1/e 2 peak intensity) in diameter.…”
Section: Methodsmentioning
confidence: 99%
“…Since the first experimental demonstration of laser and subsequent development of mode-locking and dispersion compensation techniques [1][2][3], there has been never ending quest [4][5] to generate laser pulses with increasing pulse energy, decreasing pulse duration with controlled space-time profiles and at higher pulse repetition rate for variety of scientific investigations and applications [6][7][8][9][10] e.g. generation of secondary sources of charged and neutral particles, THz to x-rays, coherent broadband sources in visible and IR range of electromagnetic radiation, modification of surface and bulk properties of optical materials etc.…”
Section: Introductionmentioning
confidence: 99%