使用溶液前驱体激光掺杂 n 型 4H-SiC 中的硼,以实现中波红外光学特性

Gunjan Kulkarni, Yahya Bougdid, C. Sugrim, Ranganathan Kumar, Aravinda Kar
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摘要

本研究报道了使用脉冲 Nd:YAG 激光器(λ = 1064 nm)在 n 型 4H 碳化硅(SiC)半导体衬底中激光掺杂硼(B)的情况。硼酸水溶液被用作硼前驱体。利用一个简单的理论传热模型来选择激光加工参数,即激光功率和激光与基片的相互作用时间,并确定掺杂 4H-SiC 基片的适当温度。所选的加工参数确保激光与基底相互作用区的温度低于碳化硅的包晶温度,以防止碳化硅发生任何晶相转变。傅立叶变换红外光谱法用于测定未掺杂和掺硼的 4H-SiC 基底在中波红外(MWIR)波长范围(3-5 μm)内的光学特性。硼原子在 4H-SiC 带隙价带上方 0.29 eV 处产生一个受体能级,对应于 λ = 4.3 μm。掺硼的 4H-SiC 衬底在中波红外范围内反射率降低,吸收率增加。掺杂基底在 λ = 4.3 μm 处检测到一个吸收峰。这证实了在 4H-SiC 带隙中产生了受体能级,因此在 4H-SiC 中掺入了硼。激光掺杂硼后,n 型 4H-SiC 的折射率明显下降,即从 2.87 降至 2.52。
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Laser doping of n-type 4H-SiC with boron using solution precursor for mid-wave infrared optical properties
Laser doping of n-type 4H-silicon carbide (SiC) semiconductor substrates with boron (B) using a pulsed Nd:YAG laser (λ = 1064 nm) is reported. An aqueous boric acid solution was used as a boron precursor. A simple theoretical heat transfer model was employed to select the laser processing parameters, i.e., laser power and laser-substrate interaction time, and determine the appropriate temperature to dope 4H-SiC substrates. The selected processing parameters ensured that the temperature at the laser-substrate interaction zone was below the SiC peritectic temperature to prevent any crystalline phase transformations in SiC. Fourier-transform infrared spectrometry was conducted to determine the optical properties of both undoped and boron-doped 4H-SiC substrates within the mid-wave infrared (MWIR) wavelength range (3–5 μm). Boron atoms create an acceptor energy level at 0.29 eV above the valence band in the 4H-SiC bandgap, which corresponds to λ = 4.3 μm. Boron-doped 4H-SiC substrate exhibited reduced reflectance and increased absorptance for the MWIR range. An absorption peak at λ = 4.3 μm was detected for the doped substrate. This confirmed the creation of the acceptor energy level in the 4H-SiC bandgap and, thus, doping of 4H-SiC with boron. A notable decrease in the refractive index, i.e., from 2.87 to 2.52, after laser doping of n-type 4H-SiC with boron was achieved.
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