• Proceedings of the Optical Society of Korea Conference
• /
• 2005.02a
• /
• pp.148-149
• /
• 2005

• Proceedings of the KIEE Conference
• /
• 1989.07a
• /
• pp.651-654
• /
• 1989

A rate equation model describing the ultrashort pulse formation is presented. The temporal and energy behavior of the distributed feedback dye laser predicted by the model has been compared the earlier papers on DFDL's. The observed good agreement allows application of the theoretical model for picosecond laser.

• Proceedings of the Optical Society of Korea Conference
• /
• 1995.06a
• /
• pp.177-184
• /
• 1995

피고초 및 펨퍼초 펄스를 얻기 위한 동기형(Synchrous mode-locking) 및 혼합형 모드결합(Hybrid mode-locking) 방식이 색소레이저에서의 출력특성에 대하여 연구하였다. 피고초 및 펨퍼스 펄스의 발생원리에 대하여 논하고, 군속도 분산과 자기위상변조와 같은 펨퍼토 펄스의 형성원리 사이의 연관성에 대하여 논한다. 또한 펨도초 펄스의 시분해 응용으로 축퇴 4광파 혼합법으로 미소반도체 CdSSe(Re645)에서 위상이완시간(Dephasing time)의 측정에 관하여 논한다.

• 기계와재료
• /
• v.22 no.4
• /
• pp.52-57
• /
• 2010

최근 극초단 펄스(ultrashort pulse) 레이저의 고출력화와 안정화가 실현되면서 본격적인 산업적 응용을 지향하는 상용 제품들이 쏟아져 나오고 있다. 극초단 펄스 레이저의 특성을 가장 잘 활용할 수 있는 적용 분야 중 하나가 유리 기판을 비롯한 투명 광학재질과 취성재료의 가공이며, 이는 시장 전망이 밝은 디스플레이와 의료 산업과 맞물려 큰 주목을 받고 있다. 본 고에서는 현재 큰 관심을 받는 분야 중 하나인 극초단 펄스 레이저를 이용한 유리 기판의 접합 기술의 원리와 최신 해외 연구 동향에 대해 살펴보고, 앞으로ㅢ 발전 방향에 대해 전망 하고자 한다.

• Proceedings of the Optical Society of Korea Conference
• /
• 2002.11a
• /
• pp.294-295
• /
• 2002

• Current Optics and Photonics
• /
• v.6 no.4
• /
• pp.407-412
• /
• 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.

• The Journal of Korean Institute of Electromagnetic Engineering and Science
• /
• v.20 no.2
• /
• pp.208-214
• /
• 2009

A design and its experimental result of a wideband self-complementary spiral antenna for UWB USPR(Ultrashort-Pulse Radar) system applications is presented. By utilizing the planar-type ultra-wideband microstrip-to-CPS balun, ultra-wideband characteristics of the inherent spiral antenna are retrieved. Also, the design procedure of the spiral antenna is simplified by performing simple impedance matching between separately designed balun and antenna. The proposed spiral antenna is equiangular self-complementary spiral antenna. The implemented antenna demonstrates widebaad performance for frequency ranges from 2.9 to 12 GHz with the relatively flat antenna gain of 2.7 to 5.3 dB and broad beamwidth of more than $70^{\circ}$. From these result, the possibility of a spiral antenna using a ultra-wideband microstrip-CPS balun is verified.

• Korean Journal of Radiology
• /
• v.22 no.5
• /
• pp.782-791
• /
• 2021

Objective: To evaluate the signal intensity of the periosteum using ultrashort echo time pulse sequence with three-dimensional cone trajectory (3D UTE) with or without fat suppression (FS) to distinguish from artifacts in porcine tibias. Materials and Methods: The periosteum and overlying soft tissue of three porcine lower legs were partially peeled away from the tibial cortex. Another porcine tibia was prepared as three segments: with an intact periosteum outer and inner layer, with an intact periosteum inner layer, and without periosteum. Axial T1 weighted sequence (T1 WI) and 3D UTE (FS) were performed. Another porcine tibia without periosteum was prepared and subjected to 3D UTE (FS) and T1 WI twice, with positional changes. Two radiologists analyzed images to reach a consensus. Results: The three periosteal tissues that were partially peeled away from the cortex showed a high signal in 3D UTE (FS) and low signal on T1 WI. 3D UTE (FS) showed a high signal around the cortical surface with an intact outer and inner periosteum, and subtle high signals, mainly around the upper cortical surfaces with the inner layer of the periosteum and without periosteum. T1 WI showed no signal around the cortical surfaces, regardless of the periosteum state. The porcine tibia without periosteum showed changes in the high signal area around the cortical surface as the position changed in 3D UTE (FS). No signal was detected around the cortical surface in T1 WI, regardless of the position change. Conclusion: The periosteum showed a high signal in 3D UTE and 3D UTE FS that overlapped with artifacts around the cortical bone.

• Journal of the Korean Institute of Illuminating and Electrical Installation Engineers
• /
• v.24 no.3
• /
• pp.20-26
• /
• 2010

In ultrashort-pulse reflectometry (USPR), a chirped waveform transformed from the USPR source impulse signal via waveguide makes it possible to employ millimeter-wave mixers for the frequency up-conversion process. Consequently, the frequency bandwidth of the USPR system is sufficiently wide to cover a large portion of the electron density profile of the plasma. Some physical aspects of the chirped waveform, such as maximum amplitude and length, are critical factors to determine the performance of the system. In this paper, the propagation of the USPR impulse signal through a rectangular waveguide is numerically studied to derive the chirped waveform using the impulse response of the waveguide. The results of numerical computation show that the chirped waveform significantly depends on the waveguide cutoff frequency as well as the waveguide length.

• Journal of the Korean Society of Manufacturing Technology Engineers
• /
• v.21 no.3
• /
• pp.382-386
• /
• 2012

A femtosecond laser with 775nm central wavelength and 150 fs of temporal pulse width was used for multi layered glass cutting applications. Ultrashort pulse was effectively used for clean glass cutting with $50{\mu}m$ depth and minimum cutting width. Laser beam was split to two stages and focused on the top surfaces of each layer. Ablation threshold of used glass was measured to be $2.59J/cm^2$. In experiments, 200mW laser power and 1mm/s scanning speed was used for preliminary experiment. Air gap was the major defect occurring parameter and laser power was less sensitive to glass cutting in the experiment. The maximum cutting speed was measured to be 60mm/min with 2kHz, however, Maximum 3m/min cutting speed can be achievable with a commercially available laser with 100kHz.