• 대한기계학회논문집B
• /
• 제30권4호
• /
• pp.350-357
• /
• 2006

A new valveless micropump for bi-directional application has been developed and tested. The micropump was fabricated on silicon and glass substrates by micromachining process. The micropump in this study consists of a membrane actuator, a pumping chamber, fluidic channels and two piezoelectric ceramic films. The channels and pumping chamber were etched on a glass wafer and the membrane was made on a silion wafer which is actuated by a piezoelectric ceramic (PZT) film. The geometry of the micropump was optimized by numerical analysis and the performance of the micropump was investigated by the experiments. The maximum flow rate was $323{\mu}L/min$ and the maximum back pressure was 294 Pa when the membrane actuator of $10{\times}10mm^2$ was driven at 130 Hz and 385 V.

• 한국광학회지
• /
• 제32권4호
• /
• pp.187-194
• /
• 2021

본 논문에서는 주 증폭기가 양방향 펌핑 방식인 MOPA (master oscillator power amplifier) 협대역 고출력 광섬유 레이저를 제작하였으며, 제작된 레이저의 출력 특성을 연구하였다. 이터븀이 도핑된 코어 25 ㎛, 클래드 400 ㎛ 편광 유지 광섬유를 사용하여 주 증폭부를 제작하였으며, 신호 광원은 PRBS (pseudo-random binary sequence) 신호에 의해 위상 변조된 3 GHz, 10 GHz의 선폭을 갖는 광원을 사용하였다. 3 GHz의 선폭을 가진 신호 광원을 이용하여 순방향과 역방향 펌프 비율을 조절하며 SBS (stimulated Brillouin scattering) 특성을 분석하였다. 10 GHz의 선폭을 가진 신호 광원을 이용하여 주 증폭기의 펌핑 비율에 따른 TMI 특성을 분석하였다. 순방향 및 역방향 펌프 비율을 1.6:1로 입사시켰을 때 주 증폭기의 출력을 1 kW까지 증폭하였으며, 기울기 효율과 빔 품질(M²)은 각각 80%, 1.36으로 측정되었다.

• Journal of the Optical Society of Korea
• /
• 제1권1호
• /
• pp.5-9
• /
• 1997

Energy transfer direction in $Er^{3+}-Tm^{3+}$-codoped fluorozirconate glasses has been studied. For $Er^{3+}-Tm^{3+}$-codoped glasses, the dependence of the green emission intensity on the pump power (Pex) of 800 nm has ranged from (Pex)$^2$ to (Pex)$^3$. From this multistep absorption, a 1.48 $\mu m$ emission from the $^3F_4{\rightarrow}^3H_4$ transition on Tm$^{3+}$ ion has been found to transfer into $^4I_{13/2}$, $^4I_{9/2}$ and $^4S_{3/2}$ on $Er^{3+}$ ion. In case of the 1.06 $\mu m$ pumping, the emissin ratio of $^3H_4$ level in $Tm^{3+}$ to $^4I_{13/2}$ in $Er^{3+}$ showed that the amount of the energy transfer from $Tm^{3+}$ into $Er^{3+}$ increased with the increasing concentration of $Tm^{3+}$ ion. Our two kinds of pumping scheme suggest that the direction of dominant energy transfer between $Er^{3+}$ and $Tm^{3+}$ should be dependent on whether the $^3F_4$ level resonates in $Tm^{3+}$ the level or not.