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中国物理学会期刊

石墨烯/4H-SiC α探测器“死层”抑制机理及原理样机表征

Mechanism of dead layer suppression in graphene/4H-SiC α-particle detector and characterization of prototype device

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  • 针对传统4H-SiC α粒子探测器金属电极“死层”较厚导致能量分辨率受限的问题, 本文采用单原子层厚石墨烯作为肖特基接触电极及入射窗, 以抑制“死层”效应. SRIM模拟显示, 100 nm厚Ni, Au电极对241Am α 粒子的垂直入射能损分别约38.36 keV, 43.50 keV, 且能损随入射角增大显著上升, 而石墨烯电极能损始终低于0.04 keV. Geant4模拟进一步显示, 当 α 粒子在0—π/3圆锥半角立体角均匀入射时, Ni, Au电极“死层”对能量分辨率的贡献分别为0.37%和0.46%, 约占4H-SiC α探测器典型能量分辨率(~1%)的37%, 46%, 而石墨烯电极的贡献仅占0.03%, 证实其可显著降低“死层”引起的能损及峰展宽. 采用PMMA辅助湿法转移工艺将石墨烯转移至4H-SiC表面, 构建探测器原理样机. 拉曼光谱证实石墨烯成功转移至4H-SiC外延表面; 器件表现出优良的整流特性及较低的漏电流; 在241Am辐照下获得清晰的α能谱峰, 空气中能量分辨率约为4.64%. 实验验证了石墨烯可作为4H-SiC肖特基电极应用于α粒子探测. 本工作为后续研制高能量分辨率石墨烯/4H-SiC α探测器奠定了基础.

     

    To address the “dead layer” effect in conventional 4H-SiC α-particle detectors, where thick metal Schottky electrodes (typically tens to hundreds of nanometers) cause substantial energy loss of incident α particles and significantly degrade energy resolution, this study proposes an innovative design that employs atomically thick graphene as both the Schottky contact electrode and the entrance window. This approach aims to effectively suppress dead-layer energy loss and enhance detector energy resolution. The investigation begins with SRIM simulations to evaluate the energy-loss characteristics of various electrode materials for 5.486 MeV α particles from a 241Am source. For 100 nm-thick Ni and Au electrodes, the energy losses at normal incidence are 38.36 keV and 43.50 keV, respectively, and increase sharply with incident angle. In contrast, graphene electrodes exhibit energy losses consistently below 0.04 keV. Subsequently, Geant4 simulations of α-particle energy deposition spectra under uniform incidence within a conical solid angle (half-angle 0–π/3) indicate that the dead-layer contributions from Ni and Au electrodes to energy resolution are 0.37% and 0.46%, respectively (accounting for 37% and 46% of the typical ~1% energy resolution for 4H-SiC α detectors), whereas graphene’s contribution is only 0.03%, quantitatively confirming its capacity to substantially reduce spectral peak broadening caused by energy loss. Experimentally, monolayer graphene grown by chemical vapor deposition (CVD) is transferred onto the surface of a 4H-SiC epitaxial layer using a PMMA-assisted wet transfer process, resulting in a graphene/4H-SiC Schottky α-detector prototype. Raman spectroscopy confirms successful high-quality graphene transfer, as evidenced by prominent G and 2D peaks, and electrical measurements demonstrate excellent rectifying characteristics and low noise levels. Irradiation experiments with a 241Am α source conducted in air produces a clear α energy spectrum peak near 5.4 MeV (after accounting for air-gap energy loss), achieving an energy resolution of 4.64% (closely matching the Geant4-simulated value of 4.22%) and validating the composite spectral structure in which some α particles achieve near-full energy deposition. The core innovation of this work lies in the integrated validation through SRIM/Geant4 simulations, device fabrication, and α-spectrum testing, which quantitatively elucidates the mechanism by which graphene electrodes suppress dead-layer energy loss and demonstrates their feasibility as ultrathin entrance-window Schottky electrodes for 4H-SiC α detectors. This research establishes a robust theoretical and experimental foundation for the future development of high-energy-resolution graphene/4H-SiC α detectors suitable for high-temperature and high-radiation environments, while offering new pathways for electrode optimization in wide-bandgap semiconductor radiation detectors.

     

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