Gładysiewicz-Kudrawiec Marta, Żak Mikołaj, Trzeciakowski Witold
Department of Experimental Physics, Faculty of Fundamental Problems of Technology, Wrocław University of Science and Technology, Wybrzeże Wyspiańskiego 27, 50-370 Wrocław, Poland.
Institute of High Pressure Physics, Polish Academy of Sciences, Sokołowska 29/37, 01-142 Warszawa, Poland.
Nanomaterials (Basel). 2025 Jan 23;15(3):174. doi: 10.3390/nano15030174.
We analyze theoretically an InGaN/GaN diode with a single quantum well supporting only one bound state. The bottom parts of the diode, namely the first barrier and the quantum well, are heavily n-doped with silicon at 5 × 10 cm to ensure a high electron concentration in the well. The voltage drop in the diode occurs in the second AlGaN barrier, which is undoped, and structure ends with a p-doped GaN. The band structure of the diode is calculated by a Schrodinger-Poisson drift-diffusion solver. Next, we calculate the absorption from the bound state in the well to the "continuum" above the well. We show the oscillatory behavior of the spectrum, with the amplitude decreasing with more negative voltage applied to the diode. Oscillations are due to interferences of the wavefunctions between the edges of the well and the slope of the potential barrier.
我们从理论上分析了一种具有单量子阱且仅支持一个束缚态的氮化铟镓/氮化镓二极管。二极管的底部部分,即第一势垒和量子阱,用硅进行了重n型掺杂,掺杂浓度为5×10¹⁹ cm⁻³,以确保量子阱中有高电子浓度。二极管中的电压降发生在未掺杂的第二氮化铝镓势垒中,结构以p型掺杂的氮化镓结束。二极管的能带结构由薛定谔 - 泊松漂移 - 扩散求解器计算得出。接下来,我们计算从量子阱中的束缚态到阱上方“连续区”的吸收。我们展示了光谱的振荡行为,随着施加到二极管上的负电压增加,振幅减小。振荡是由于量子阱边缘与势垒斜率之间波函数的干涉引起的。