• 전자공학회논문지A
• /
• 제33A권7호
• /
• pp.185-197
• /
• 1996

We have adopted the strain compensated PBH(planar buried heterostructure) - LD in which the MQW active layer consisted of 1.4% compressively strained GainAsP (E$_{g}$ = 0.905eV) wells and 0.7% tensile strained GaInAsP(E$_{g}$ = 1.107eV) barriers grown by metal organic vapor phase epitaxy (MOVPE). We hav einvestigated effects of number of wells and the structure of the separate confinement heterostructure (SCH) layer in the strain-compensated MQW-PBH-LD. The threshold current, the external quantum efficiency, the transparency current density J$_{o}$, and the gain constant .beta. have been evaluated for uncoated MQW-PBH-LD. As the number of wells increases, the internal quantum efficiency and the transparency current density decreases, whereas the gain contant increases. The small width of the SCH layer shows the large internal quantum efficiency. The small internal loss and the large gain constant have been obtained by inserting the large bandgap SCH layer.

• ETRI Journal
• /
• 제13권4호
• /
• pp.2-9
• /
• 1991

Buried-heterostructure lasers are more difficult to fabricate than weakly index guided or gain guided lasers. However, these strongly index guided structures are most suitable for a source of lightwave transmission systems. But, for conventional etched mesa buried heterostructure lasers, the regrowth of InP blocking layer is difficult and irreproducible. So, there are inevitable leakage currents flowing outside the active region resulting poor performance. To eliminate these problems, we used a planar buried heterostructure. As a results, the average threshold current was 28mA and the differential quantum efficiency was about 20% per facet for $1.3\mum$ GaInAsP/InP PBH-LD. The initial forward leakage current was not exceeding $1\muA$ and the reverse voltage for $-10\muA$ was -3V~-5V, these are improved figure of 1mA~10mA and -1V~-3V for EMBH laser diode. The chip modulation bandwidth was more than 2.4GHz for $1.5I_th$.

• Journal of Korean Vacuum Science & Technology
• /
• 제4권3호
• /
• pp.81-85
• /
• 2000

The effects of $NH_3$ flow rate and reactor pressure on Al composition and the interface of AlGaN/GaN heterostructure were studied. Equilibrium partial pressure of Ga and Al over AiGaN alloy was calculated as a function of growth pressure, $NH_3$flow rate and temperature. It was found equilbrium vapor pressure of Al is significantly lower than that of Ga, thus, the alloy composition mainly controlled by Ga partial pressure. We believe that more decomposition of Ga occur at lower $NH_3$ flow rate and higher growth pressure leads to preferred Al incorporation into AlGaN. The alloy composition gradient became larger at AlGaN/GaN heterointerface at higher reactor pressures, higher Al composition and low $NH_3$ flow rate. This composition gradient lowered sheet carrier concentration and electron mobility as well. We obtained an AlGaN/GaN heterostructure with sheet carrier density of ${\sim}2{\times}10^{13}cm^{-2}$ and mobility of 1250 and 5000 $cm^2$/Vs at 300 K and 100 K, respectively.

• 한국재료학회지
• /
• 제33권6호
• /
• pp.229-235
• /
• 2023

An all-perovskite oxide heterostructure composed of SrSnO₃/Nb-doped SrTiO₃ was fabricated using the pulsed laser deposition method. In-plane and out-of-plane structural characterization of the fabricated films were analyzed by x-ray diffraction with θ-2θ scans and φ scans. X-ray photoelectron spectroscopy measurement was performed to check the film's composition. The electrical transport characteristic of the heterostructure was determined by applying a pulsed dc bias across the interface. Unusual transport properties of the interface between the SrSnO₃ and Nb-doped SrTiO₃ were investigated at temperatures from 100 to 300 K. A diodelike rectifying behavior was observed in the temperature-dependent current-voltage (IV) measurements. The forward current showed the typical IV characteristics of p-n junctions or Schottky diodes, and were perfectly fitted using the thermionic emission model. Two regions with different transport mechanism were detected, and the boundary curve was expressed by ln I = -1.28V - 13. Under reverse bias, however, the temperature- dependent IV curves revealed an unusual increase in the reverse-bias current with decreasing temperature, indicating tunneling effects at the interface. The Poole-Frenkel emission was used to explain this electrical transport mechanism under the reverse voltages.

• 한국재료학회:학술대회논문집
• /
• 한국재료학회 2007년도 추계학술발표대회 및
• /
• pp.102.2-102.2
• /
• 2007

• 한국재료학회:학술대회논문집
• /
• 한국재료학회 1992년도 춘계학술발표회
• /
• pp.121-122
• /
• 1992

• 한국광학회:학술대회논문집
• /
• 한국광학회 1999년도 제16회 광학 및 양자전자 학술발표회Proceedings of 16th Optics and Quantum Electronics Conference, 1999
• /
• pp.86-87
• /
• 1999

• 한국재료학회지
• /
• 제5권4호
• /
• pp.420-425
• /
• 1995

AlGaN/GaInN 이중이종접합구조(double heterostructure :DH)를 대기압 유기금속기상에 피텍셜(MOVPE)법으로 AIN 와충층을 이용하여 사파이어 기판위에 성장하고, 실온에서의 광여기법에 의한 청색영역의 단면모드 유도방출특성과 편광특성을 조사하였다. 여기광원의 광밀도가 증가함에 따라 청색 영역에서의 유도방출 피크는 낮은 에너지 쪽으로 이동하였고, 유도방출 피크파장은 여기광밀도가 200kW/$cm^{2}$일때 402nm 이었으며, 스펙트럼의 반치폭은 18meV 이었다. 또한 유도방출에 필요한 여기광밀도의 임계치는 130 kW/$cm^{2}$ 이었다. AlGaN/GaInN로부터 방출되는 유도방출 광은 임계치 이상에서 TE-mode로 편광 되었다.

• 한국재료학회지
• /
• 제5권4호
• /
• pp.445-450
• /
• 1995

AIN 완충층을 이용하여 대기압 유기금속에피텍셜 (MOVPE)법으로 사파이어 기판위에 성장시킨 AlGaN/GaN 이중 이종접합구조(double heterostructure : DH)의 고밀도 광여기에 의한 자외선 영역에서의 단면모드 유도방출 특성에 대하여 조사하였다. 실온에서 여기광 밀도 200kW/$cm^{2}$에서 방출된 AlGaN/GaN DH의 유도방출 피크파장과 반치폭은 각각 369nm와 22.4meV이었으며, 80K의 온도에서는 각각 360.1nm와 13.4meV이었다. 고밀도 광여기에 의하여 단면모드 자외영역 유도방출을 얻기에 필요한 입사광 밀도의 임계치는 실온과 80K의 온도에서 각각 89kW/$cm^{2}$와 44kW/$cm^{2}$이었다.

• 한국세라믹학회지
• /
• 제30권3호
• /
• pp.206-214
• /
• 1993

Coherent precipitation of Zn3P2 during Zn diffusion in a GaInAsP/InP heterostructure was studied using high-resolution transmission electron microscopy. Zn-diffusion-induced intermixing of Ga and In across the GaInAsP/InP heterointerface provided a Ga-mixed InP region which was nearly lattice-matched with Zn3P2 crystal and thus allowed thecoherent precipitation of Zn3P2. The Zn3P2 precipitates were preferentially nucleated at stacking faults which were formed to relax interfacial strain built up by the intermixing. The precipitates were grown to planar epitaxial layer along (100) plane in the lattice-matched region. The TEM images and diffraction pettern revealed that the tetragonal Zn3P2 crystals were coherently matched to the fcc structured GaInP matrix by the {{{{ SQRT {2} $\times$ SQRT {2} $\times$2 }} arrangement. The precipitation reaction of Zn3P2 was explained by an atomic migration model based on the kick-out mechanism.