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中国物理学会期刊

重离子在碳化硅中的输运过程及能量损失

CSTR: 32037.14.aps.70.20210503

Transport process and energy loss of heavy ions in silicon carbide

CSTR: 32037.14.aps.70.20210503
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  • 利用蒙特卡罗方法, 模拟计算了不同线性能量传输(liner energy transfer, LET)的重离子在碳化硅中的能量损失, 模拟结果表明: 重离子在碳化硅中单位深度的能量损失受离子能量和入射深度共同影响; 能量损失主要由初级重离子和次级电子产生, 非电离能量损失只占总能量损失的1%左右; 随着LET的增大, 次级电子的初始角度和能量分布越来越集中; 重离子诱导产生的电荷沉积峰值位置在重离子径迹中心, 在垂直于入射深度方向上呈高斯线性减小分布. 利用锎源进行碳化硅MOSFET单粒子烧毁试验, 结合TCAD模拟得到不同漏极电压下器件内部电场分布, 在考虑电场作用的蒙特卡罗模拟中发现: 碳化硅MOSFET外延层的电场强度越大, 重离子受电场作用在外延层运动的路径越长、沉积能量越多, 次级电子越容易偏向电场方向运动导致局部能量沉积过高.

     

    Using the Monte Carlo method, the energy losses in silicon carbide of heavy ions with different linear energy transfers (LETs) are simulated and calculated. The simulation results show that the energy loss per unit depth of heavy ions in silicon carbide is affected by both the ion energy and the incident depth. Primary heavy ions and secondary electrons mainly cause energy loss, and the non-ionization energy loss only accounts for about 1% of the total energy loss. With the increase of LET, the initial angle and energy distribution of the secondary electrons become more and more concentrated. The peak position of the generated charge deposition is in the center of the heavy-ion track, and the distribution is linearly decreasing in Gaussian form in the direction perpendicular to the incident depth. In the californium source experiment of SiC MOSFET, when the drain voltage is 480 V, the device has a single event burnout, and the breakdown voltage of SiC MOSFET is less than 1 V after burnout has occurred. With the experimental results, we carry out the TCAD simulation of SiC MOSFET and obtain the electric field distribution inside the device under different drain voltages. The electric field parameters are used in the Monte Carlo simulation of SiC MOSFET with considering the metal layer. It is found in the Monte Carlo simulation that the greater the electric field of the epitaxial layer, the longer the path of heavy ions moving on the epitaxial layer is and the more the deposited energy, and that the secondary electrons are more likely to move in the direction of the electric field as the electric field increases, resulting in excessive energy deposition in local areas.

     

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