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中国物理学会期刊

AlGaAs电子阻挡层组分优化对980 nm半导体激光器温度特性的影响研究

Study on the Effect of Composition Optimization of AlGaAs Electron Blocking Layers on the Temperature Characteristics of 980 nm Semiconductor Lasers

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  • 针对980 nm边发射半导体激光器在高温下因电子热逃逸导致的性能退化问题,本文通过能带工程,在P面波导层与势垒层之间设计了不同组分的AlGaAs电子阻挡层(EBL)。利用PICS 3D软件,系统性仿真对比了无EBL、Al0.3GaAs EBL及Al0.4GaAs EBL三种结构在300-360 K温区内的光电特性。研究结果表明,EBL能显著抑制电子泄漏,其中Al0.4GaAs EBL在360 K下将P型包层电子浓度降低了97.14%。然而,该结构过高的Al组分会引入大量的空穴注入势垒,导致有源区载流子严重失衡,量子阱内电子浓度反常升高至2.3×1018 cm-3,进而引发强烈的俄歇复合,劣化了激光器高温下的阈值特性与输出功率。相比之下,Al0.3GaAs EBL在电子限制与空穴注入之间取得了最佳平衡,其在全温域内表现出最优的综合性能:在保证94.7%的电子抑制效果的同时,具有280.9 K的最高特征温度T0,并且相比于其他两种结构,光功率的仿真值也是最高,为3.693 W。研究发现,EBL设计的核心在于寻求载流子限制与注入效率的全局最优,而非单一追求极高的势垒,该结论为研制高温度稳定性的980 nm泵浦激光器提供了关键的设计依据。

    High-power 980 nm edge-emitting semiconductor lasers (EELs) serve as the dominant pump sources for erbium-doped fiber amplifiers (EDFAs) and are crucial for various industrial, medical, and photonic integration applications. However, their performance severely degrades at elevated temperatures, primarily due to enhanced electron thermionic escape from the active region, leading to increased threshold current, reduced output power, and limited reliability. This work aims to address this fundamental challenge by strategically designing and optimizing an AlGaAs Electron Blocking Layer (EBL) within the P-side of the laser heterostructure. The core objective is to systematically investigate the influence of EBL aluminum (Al) composition on the carrier dynamics, recombination mechanisms, and resultant temperature-dependent electro-optical characteristics of 980 nm EELs, thereby identifying the optimal design paradigm for achieving superior high-temperature stability.
    A comprehensive numerical simulation study was conducted using the commercial semiconductor device simulator PICS 3D, which self-consistently solves the coupled electrical, optical, and thermal equations. Three distinct epitaxial structures were designed and compared: 1) a Reference structure without an EBL; 2) a structure incorporating a 10 nm Al0.3GaAs EBL; and 3) a structure incorporating a 10 nm Al0.4GaAs EBL. The EBL was positioned between the undoped P-side waveguide and the barrier layer. The active region consisted of an 8 nm In0.2Ga0.3As single quantum well with GaAsP0.03 barriers. The cladding layers employed a graded Al-composition AlGaAs design. Simulations were performed over a temperature range of 300 K to 360 K for devices with a 25 μm stripe width and a 2 mm cavity length. Key analyzed parameters included spatial carrier distributions (electron/hole concentrations), radiative and Auger recombination rates, power-current-voltage (P-I-V) characteristics, threshold current (Ith), characteristic temperature (T0), and lasing wavelength shift.
    Carrier Confinement and Injection Balance: The introduction of an AlGaAs EBL dramatically suppressed electron leakage into the P-cladding. At 360 K, the peak electron concentration in the P-cladding was reduced by 94.7% for the Al0.3GaAs EBL and by 97.14% for the Al0.4GaAs EBL, compared to the reference structure. However, the higher Al-content EBL (Al0.4GaAs) introduced a significantly larger valence band barrier, severely impeding hole injection into the quantum well (QW). This imbalance caused an anomalous accumulation of electrons within the QW, reaching a density of 2.3×1018 cm-3 at 360 K for the Al0.4GaAs EBL, compared to 1.72×1018 cm-3 for the Al0.3GaAs EBL and 1.81×1018 cm-3 for the reference structure.
    Recombination Dynamics: The disparate carrier distributions led to distinct recombination pathways. The Al0.4GaAs EBL structure exhibited the highest radiative recombination rate due to its high electron density but simultaneously suffered from the strongest Auger recombination—36.5% higher than the reference at 360 K. This is attributed to the cubic dependence of Auger recombination on carrier density. The Al0.3GaAs EBL structure maintained a high radiative rate while effectively suppressing Auger recombination, achieving a more favorable balance.
    Threshold and Spectral Characteristics: Despite its superior electron confinement, the Al0.4GaAs EBL structure exhibited the highest threshold current across the temperature range, a direct consequence of the hole injection bottleneck and enhanced non-radiative losses. The Al0.3GaAs EBL structure achieved the best temperature stability, characterized by the highest characteristic temperature T0 = 280.9 K, compared to 271.7 K (reference) and 274.7 K (Al0.4GaAs EBL). It also demonstrated the lowest wavelength temperature drift coefficient (0.346 nm/°C), enhancing spectral stability.
    Power Output and Efficiency: The Al0.3GaAs EBL structure delivered the highest continuous-wave output power across the entire temperature range. At 360 K, its maximum power was 3.592 W, representing an 6.90% improvement over the reference structure (3.360 W). The Al0.4GaAs EBL structure showed a similar improvement (3.590 W) but at the cost of higher operating voltage at lower temperatures. The voltage-current relationship revealed a complex interplay between hole injection barrier and carrier recombination, with a crossover occurring above 350 K where the Al0.4GaAs EBL voltage became lower, indicating a shift in the dominant mechanism to leakage and recombination dynamics.
    This study elucidates the critical trade-off in EBL design for high-temperature 980 nm semiconductor lasers. While increasing the Al composition in the AlGaAs EBL strengthens electron confinement, an excessively high Al fraction (0.4) introduces a prohibitive hole injection barrier. This disrupts carrier balance in the active region, leading to electron pile-up, a dramatic increase in detrimental Auger recombination, and ultimately degrading threshold and power performance. The Al0.3GaAs EBL emerges as the optimized design, successfully striking an optimal balance between effective electron blocking and efficient hole injection. It achieves a significant suppression of electron leakage (>94%) while minimizing parasitic non-radiative losses, resulting in the best overall performance: the highest T0 (280.9 K), the lowest wavelength drift, and the greatest output power across the 300-360 K range. The findings underscore that the key to improving high-temperature laser characteristics lies not in merely maximizing the EBL barrier height but in globally optimizing the carrier confinement-injection equilibrium. This work provides essential guidelines and a theoretical foundation for the epitaxial design of temperature-stable, high-power 980 nm pump lasers.

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