基于热耦合行列复用结构的32×32NbN SNSPD阵列

IF 5.6 Q1 ENGINEERING, ELECTRICAL & ELECTRONIC
TianZhu Zhang , You Xiao , HuiQin Yu , Jia Huang , ChaoLin Lv , LingDong Kong , XiaoYu Liu , Hao Li , LiXing You , Zhen Wang
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引用次数: 0

摘要

我们报道了一种针对近红外1550nm波长的超导纳米线单光子探测器(SNSPD)阵列,该阵列由32×32纳米线像素和0.96mm×0.96mm的面积组成。与大多数报道的具有非晶膜的大规模SNSPD阵列不同,我们的阵列中使用了NbN超导纳米线,这允许探测器在2.3 K下运行,由紧凑的两级Gifford–McMahon低温冷却器提供。在我们的阵列中采用了热耦合行-列复用,以避免在电耦合行-柱架构中发生电流再分配和电信号损失。所制造的探测器阵列在1550nm和405nm处分别显示出94%的像素产率和77%和96%的最大本征效率。还研究了定时抖动和热耦合概率。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
32 × 32 NbN SNSPD array based on thermally coupled row-column multiplexing architecture

We report a superconducting nanowire single-photon detector (SNSPD) array aiming for a near-infrared 1550-nm wavelength that consists of 32 × 32 nanowire pixels and an area of 0.96 mm × 0.96 mm. Unlike most reported large-scale SNSPD arrays with amorphous films, NbN superconducting nanowires are employed in our array, which allows the detector operation at 2.3 K provided by a compact two-stage Gifford–McMahon cryocooler. Thermally coupled row–column multiplexing is employed in our arrays to avoid current redistribution and loss of electrical signal occurring in the electrically coupled row–column architecture. The fabricated detector array shows a pixel yield of 94% and maximal intrinsic efficiencies of 77% and 96% at 1550 nm and 405 nm, respectively. The timing jitter and the thermal coupling probability are also investigated.

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