• Title/Summary/Keyword: fs laser

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fs-laser Ablation and Optoperforation Threshold for PDMS Thin Film on $\mu$-channel (미세 유체 상 PDMS 고분자 필름의 펨토초 레이저 어블레이션 및 천공 임계치 연구)

  • Woo, Suk-Yi;Sidhu, M.S.;Yoon, Tae-Oh;Jeoung, Sae-Chae;Park, Il-Hong
    • Journal of the Korean Society for Precision Engineering
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    • v.27 no.2
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    • pp.29-33
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    • 2010
  • We have investigated fs-laser ablation as well as optoperforation threshold of PDMS (Polydimethylsiloxane) thin lid cover on ${\mu}$-channel with changing the flow medium from water to hemoglobin. The ablation threshold is found to be independent of both PDMS thin film thickness and flow medium, but the optoperforation threshold is dependent on the films thickness. The observation that the ablation process is well described with simple two-temperature model supposed that the cover lid PDMS of $\mu$-channel be processed with minimized thermal effects by fs-laser with low laser fluence.

Enamel pretreatment with Er:YAG laser: effects on the microleakage of fissure sealant in fluorosed teeth

  • Memarpour, Mahtab;Kianimanesh, Nasrin;Shayeghi, Bahareh
    • Restorative Dentistry and Endodontics
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    • v.39 no.3
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    • pp.180-186
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    • 2014
  • Objectives: The purpose of this in vitro study was to evaluate the microleakage and penetration of fissure sealant in permanent molar teeth with fluorosis after pretreatment of the occlusal surface. Materials and Methods: A total of 120 third molars with mild dental fluorosis were randomly divided into 6 groups (n = 20). The tooth surfaces were sealed with an unfilled resin fissure sealant (FS) material. The experimental groups included: 1) phosphoric acid etching (AE) + FS (control); 2) AE + One-Step Plus (OS, Bisco) + FS; 3) bur + AE + FS; 4) bur + AE + OS + FS; 5) Er:YAG laser + AE + FS; and 6) Er:YAG laser + AE + OS + FS. After thermocycling, the teeth were immersed in 0.5% fuchsin and sectioned. Proportions of mircoleakage (PM) and unfilled area (PUA) were measured by digital microscope. Results: Overall, there were significant differences among all groups in the PM (p = 0.00). Group 3 showed the greatest PM, and was significantly different from groups 2 to 6 (p < 0.05). Group 6 showed the lowest PM. Pretreatment with Er:YAG with or without adhesive led to less PM than bur pretreatment. There were no significant differences among groups in PUA. Conclusions: Conventional acid etching provided a similar degree of occlusal seal in teeth with fluorosis compared to those pretreated with a bur or Er:YAG laser. Pretreatment of pits and fissures with Er:YAG in teeth with fluorosis may be an alternative method before fissure sealant application.

High-power SESAM Mode-locked Yb:KGW Laser with Different Group-velocity Dispersions

  • Park, Byeong-Jun;Song, Ji-Yeon;Lee, Seong-Yeon;Yee, Ki-Ju
    • Current Optics and Photonics
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    • v.6 no.4
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    • pp.407-412
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    • 2022
  • We report on a diode-laser-pumped mode-locked Yb:KGW laser system, which delivers ultrashort pulses down to 89 fs at a repetition rate of 63 MHz, with an average power of up to 5.6 W. A fiber-coupled diode laser at 981 nm, operated with a compact driver, is used to optically pump the gain crystal via an off-axis parabolic mirror. A semiconductor saturable-absorber mirror is used to initiate the pulsed operation. Laser characteristics such as the pulse duration, spectrum bandwidth, and output power are investigated by varying the intracavity dispersions via changing the number of bounces between negative-dispersive mirrors within the cavity. Short pulses with a duration of 89 fs, a center wavelength of 1,027 nm, and 3.6 W of output power are produced at a group-velocity dispersion (GVD) of -3,300 fs2. As the negative GVD increases, the pulse duration lengthens but the output power at the single-pulse condition can be enhanced, reaching 5.6 W at a GVD of -6,600 fs2. Because of pulse broadening at high negative GVDs, the highest peak intensity is achievable at a moderate GVD with our system.

High Power 1.83 GHz Femtosecond Yb-doped Fiber Laser Incorporating Repetition Rate Multipliers

  • In Chul Park;Eun Kyung Park;Ye Jin Oh;Hoon Jeong;Ji Won Kim;Jeong Sup Lee
    • Current Optics and Photonics
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    • v.7 no.6
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    • pp.732-737
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    • 2023
  • A high-power Yb-doped femtosecond (fs) fiber laser at a repetition rate of 1.83 GHz is reported. By employing a 5-stage repetition rate multiplier, the repetition rate of the mode-locked master oscillator was multiplied from 57.1 MHz to 1.83 GHz. The ultrashort pulse output at 1.83 GHz was amplified in a two-stage Yb-doped fiber amplifier, leading to >100 W of fs laser output with a pulse duration of 290 fs. The theoretical pulse width along the fiber was simulated, showing that it was in good agreement with experimental results. Further improvement in power scaling is discussed.

Generation of sub-10-fs Pulses from a kerr-Iens mode-locked Ri:sapphire Iaser (Kerr 렌즈 모드록킹된 티타늄 사파이어 레이저에서 10fs 이하 펄스의 발생)

  • 홍경한;차용호;강영일;남창희
    • Korean Journal of Optics and Photonics
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    • v.11 no.1
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    • pp.43-46
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    • 2000
  • We generated 9-fs pulses from a Kerr-lens mode-locked Ti:sapphire laser only using commercial optical components. Two sets of prisms pair made of fused silica were used to compensate group delay dispersion inside and outside the laser oscillator respectively, and broadband mirrors were used to obtain a broad spectrum. By comparison between reflectance curves of the broadband mirrors and those of previous ones, broadband mirrors which have high reflectance bandwidth of over 180 nm were found to be essential to produce sub-IO-fs pulses. ulses.

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Application of a LIBS technique using femtosecond and nanosecond pulses for the CIGS films analysis (펨토초 및 나노초 레이저를 이용한 박막태양전지의 레이저 플라즈마 분광 분석)

  • Lee, S.H.;Choi, J.H.;Gonzalez, J.J.;Hou, H.;Zorba, V.;Russo, R.E.;Jeong, S.H.
    • Laser Solutions
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    • v.17 no.4
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    • pp.7-13
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    • 2014
  • In this work, the application of laser induced breakdown spectroscopy (LIBS) for the composition analysis of thin $Cu(In,Ga)Se_2$ (CIGS) solar cell films ($1-2{\mu}m$ thickness) is reported. For the ablation of CIGS films, femtosecond (fs) laser (wavelength = 343nm, pulse width = 500fs) and nanosecond (ns) laser (wavelength = 266nm, pulse width = 5ns) were used under atmospheric environment. The emission spectra were detected with an intensified charge coupled device (ICCD) spectrometer and multichannel CCD spectrometer for fs-LIBS and ns-LIBS, respectively. The calibration curves for fs-LIBS and ns-LIBS intensity ratios of Ga/Cu, In/Cu, and Ga/In were generated with respect to the concentration ratios measured by inductively coupled plasma optical emission spectrometry (ICP-OES).

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High power tunable Ti:sapphire laser with sub-40fs pulsewidth (40펨토초 미만 펄스폭의 고출력 파장가변 티타늄사파이어 레이저)

  • 임용식;노영철;이기주;김대식;장준성
    • Korean Journal of Optics and Photonics
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    • v.10 no.5
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    • pp.430-438
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    • 1999
  • We have utilized soft-aperturing by gain media to develop a high-power tunable Ti:Sapphire laser with sub-40-fs and broad tuning range. The tunable spectral range was only limited by the bandwidth of mirrors. We made use of knife-edge slits near an intra-cavity prism controlled by micro-stepping-motors to tune the center wavelength continuously. The tunability of the center wavelength was ranged from 770 nm to 870 nm, and the measured pulsewidth was sub-40 fs throughout the above spectral range. The shortest pulsewidth was about 17 fs at the center wavelength of 820 nm and the spectral bandwidth was 72 nm. At 5 W pumping power of the Ar-ion laser we obtained average output power of 440 mW~580 mW. For the cw and Kerr-lens mode-lodking conditions, we have evaluated the value of an amplitude modulation to be ${\gamma}=2.5{\times}10^{-8}/W$ from the calculated waists of a Gaussian beam on the Ti:sapphire crystal surface. Using this result we demonstrate that the generation of sub-40-fs Kerr-lens mode-locked pulse can be described by the Ginzberg-Landau model which is a weak pulse shaping model.

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Fabrication of Balanced CPM(Colliding Pulse Mode-locked) Ring Dye Laser (Balanced CPM(Colliding Pulse Mode-locked) 링 색소 레이저 제작)

  • 정영붕;김동호;이인원
    • Korean Journal of Optics and Photonics
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    • v.1 no.2
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    • pp.185-190
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    • 1990
  • Balanced CPM ring dye laser was fabricated. Pulses as short as 62 fs were measured using noncollinear second harmonic generation autocorrelator. The optimum conditions were studied by changing the concentration of staturable absorber, pumping power of Ar+ laser and alignments of the intracavity four-prism sequence.

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Characteristic of FS-laser ablation of metal thin film with respect to the variation of material and substrate (펨토초 레이저를 이용한 박막 재료 및 기판 변화에 따른 가공 특성에 관한 연구)

  • Kim B.H.;Shin H.G.;Lee J.G.;Jeong S.C.
    • Proceedings of the Korean Society of Precision Engineering Conference
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    • 2006.05a
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    • pp.671-672
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    • 2006
  • We have investigated the behavior of the ultrafast laser ablation of chromium films (200nm) on the silicon and pyrex-glass(corning 7740) substrate with respect to the laser fluence and the number of laser pulses. In addition, several experiments about ITO thin film were carried out with femto-second Ti:Sapphire laser (150fs). Finally, we introduce the ablation characteristic in accordance with materials of thin film and substrate.

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Controlled Surface Functionalities of metals using Femtosecond Laser-induced Nano- and Micro-scale Surface Structures (펨토초 레이저 유도 나노 및 마이크로 구조물을 활용한 금속 표면 기능성 제어)

  • Taehoon Park;Hyo Soo Lee;Hai Joong Lee;Taek Yong Hwang
    • Design & Manufacturing
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    • v.17 no.2
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    • pp.55-61
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    • 2023
  • With femtosecond (fs) laser pulse irradiation on metals, various types of nano- and micro-scale structures can be naturally induced at the surface through laser-matter interaction. Two notable structures are laser-induced periodic surface structures (LIPSSs) and cone/spike structures, which are known to significantly modify the optical and physical properties of metal surfaces. In this work, we irradiate fs laser pulses onto various types of metals, cold-rolled steel, pickled & oiled steel, Fe-18Cr-8Ni alloy, Zn-Mg-Al alloy coated steel, and pure Cu which can be useful for precise molding and imprinting processes, and adjust the morphological profiles of LIPSSs and cone/spike structures for clear structural coloration and a larger range of surface wettability control, respectively, by changing the fluence of laser and the speed of raster scan. The periods of LIPSSs on metals used in our experiments are nearly independent of laser fluence. Accordingly, the structural coloration of the surface with LIPSSs can be optimized with the morphological profile of LIPSSs, controlled only by the speed of the raster scan once the laser fluence is determined for each metal sample. However, different from LIPSSs, we demonstrate that the morphological profiles of the cone/spike structures, including their size, shape, and density, can be manipulated with both the laser fluence and the raster scan speed to increase a change in the contact angle. By injection molding and imprinting processes, it is expected that fs laser-induced surface structures on metals can be replicated to the plastic surfaces and potentially beneficial to control the optical and wetting properties of the surface of injection molded and imprinted products.