中国物理B ›› 2026, Vol. 35 ›› Issue (3): 38501-038501.doi: 10.1088/1674-1056/adfbd6
Qing-Xiao Ma(马卿效)1,2, Wen Zhang(张文)1,†, Pei-Zhan Li(李佩展)1, Zhi-Fa Feng(冯志发)1,2, Xian-Feng Zhou(周先锋)1,2, Zheng Wang(王争)1, Jia-Qiang Zhong(钟家强)1, Wei Miao(缪巍)1, Yuan Ren(任远)1, Jing Li(李婧)1, and Sheng-Cai Shi(史生才)1,‡
Qing-Xiao Ma(马卿效)1,2, Wen Zhang(张文)1,†, Pei-Zhan Li(李佩展)1, Zhi-Fa Feng(冯志发)1,2, Xian-Feng Zhou(周先锋)1,2, Zheng Wang(王争)1, Jia-Qiang Zhong(钟家强)1, Wei Miao(缪巍)1, Yuan Ren(任远)1, Jing Li(李婧)1, and Sheng-Cai Shi(史生才)1,‡
摘要: We present the contribution of x-ray incident-position dependence on the absorber to the energy resolution of Ti/Au transition-edge sensors (TESs). The pulse height varies with the position due to insufficient thermal conductivity and geometry of the absorber that degrades the measured energy resolution. We develop a three-dimensional (3D) electro-thermal simulation model and thoroughly study the position dependent contribution to energy resolution ($\Delta E_{\rm p}$) for two presentative absorber structures: an absorber directly deposited on the center of TES sensor (design A) and an absorber cantilevered on the TES sensor by several stems (design B). For design A with a 30 μm$\times$40 μm Au absorber $\Delta E_{\rm p}$ is found to be 9.4 eV, while it is reduced to 1.35 eV for design B with a 100 μm$\times$100 μm Au absorber. Although the contribution of position dependence is relatively small, this study facilitates further optimization of the absorber structure to achieve enhanced energy resolution.
中图分类号: (Superconducting optical, X-ray, and γ-ray detectors (SIS, NIS, transition edge))