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  • 學位論文

量子點雷射中的雙能態放光與模態反競爭

Simultaneous Two-state Lasing and Mode Anticompetition in Quantum Dot Lasers

指導教授 : 林清富

摘要


隨著量子點雷射製作的技術趨於成熟,我們對於量子點雷射的諸多特性有更多的了解。本論文中我們針對設計過後的量子點雷射,研究其雙能態放光現象與模態反競爭。 在將InAs/In0.15Ga0.85As/GaAs兩種尺寸多層量子點雷射依據標準的製程製作完成後,我們把元件黏著在散熱銅座上,架設外部共振腔,並且測量其輸出光功率對電流特性曲線、光輸出頻譜在不同電流下的變化。從測量結果我們發現在不同長度的元件當中,光輸出頻譜會發光在不同波長;在長元件當中,光輸出頻譜會出現基態放光;在短元件當中,光輸出頻譜會出現激態放光;而當長度介於長元件與短元件中間某個範圍時,雷射會出現特有的雙能態放光現象。對於雙能態放光,我們測量了操作在脈衝與直流時,光輸出頻譜在不同電流下的變化,並且觀察了基態與激態頻譜的消長趨勢,發現雙能態頻譜都會出現兩個峰值,在可調波長實驗的幫助下,證實雙能態兩個峰值間有很密切的關係;而我們也利用簡單的次線性曲線模擬了雙能態頻寬增加的趨勢。在雙能態輸出光功率對電流特性曲線上,我們利用簡單的雙能態載子、光子動態方程式模擬了光功率對電流特性曲線,最後加入文獻的探討,解釋了基態光出現的衰減現象。 在控制長波長出現的反競爭現象部份,我們經由可調波長實驗,發現當可調波長位於1235nm與1265nm時,激態頻譜會出現發光的peak。模擬在可調波長出現前後載子的變化,發現激態的載子會因為可調波長位於1235nm與1265nm,出現上升的趨勢,載子提供了増益,使激態頻譜出現發光的peak。 在控制短波長出現的反競爭現象部份,我們對元件做了抗反射鍍膜並架設雙波長,研究了三組在不同電流下的反競爭現象;最後,與之前在非對稱多重量子井中出現的反競爭現象作比較,探討主動區的差異、反競爭的異同、以及optical pumping的機制與差別。

關鍵字

量子點雷射 量子點 子井 雙能態 競爭 反競爭

並列摘要


With the improvement of the fabrication technology in quantum-dot lasers, the characteristics are further understood. In this dissertation, we focus on the phenomenon of simultaneous two-state lasing and mode anti-competition in the designed quantum-dot lasers. The InAs/In0.15Ga0.85As/GaAs laser diodes are fabricated with standard processing techniques. The fabricated devices are bonded on the copper heat sink, and their electrical and optical properties are measured. The measured results show that devices with variable lengths emit light at different wavelengths. In the longer devices, the output spectrum exhibits ground state transition; in the shorter ones, the output spectrum exhibits excited state transition; while the device length ranges between the longer ones and the shorter ones, the laser diodes exhibit simultaneous two-state lasing. Focused on this phenomenon, we observe the spectrum-versus-wavelength curves and the trends of ground state and excited state under pulsed and continued-wave operations respectively. Experimental results show that there exits two peaks in ground state and excited state separately. With the help of external cavity, we prove that the two peaks in ground state and excited state have relationship. In addition, the simple sub-linear curves are used to fit the bandwidth trends in both states under pulsed and continued-wave operation. At the end of the chapter, the two-state carrier and photon rate equations are listed to simulate the two-state light-current characteristic curves. The paper results are added after the simulation to explain the decay of the light power in the ground state. In the 1st part of mode anti-competition-controlling the long-wavelength mode, we found that the nearly lasing peak will appear corresponding to the excited state transitions when the tuning wavelengths locate at 1235nm and 1265nm in the tuning experiments using the external cavity. Simulation of the carrier distribution shows that the carriers in the excited state will increase with the feedback intensity of light at 1235nm and 1265nm from the grating in the external cavity. Carrier increase results in the gain increase in the excited state. As a result, the nearly lasing peak will appear corresponding to the excited state transitions in the output spectrum. In the 2nd part of mode anti-competition-controlling the short-wavelength mode, one facet of the device is anti-reflection (AR) coated. After coating, the device operates in the external cavity. The external cavity laser is controlled to operate at two wavelengths at 1170nm and 1250nm. Three sets of experiments are done separately under different injection currents to study the anti-competition phenomenon. Finally, we compare our results with previous experiments of anti-competition in non-identical MQW lasers. The comparison includes the difference of gain medium, the difference of anti-competition, and the difference of optical pumping in QD and QW lasers.

參考文獻


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