在0.18微米的多通道门芯片中,用于量子应用的高压CMOS
Christoph Ribisch1, Michael Hofbauer1, Seyed Saman Kohneh Poushi1
1Institute of Electrodynamics, Microwave and Circuit Engineering, Faculty of Electrical Engineering and Information Technology, Technische Universität Wien, 1040 Vienna, Austria.
Sensors (Basel, Switzerland)
|December 23, 2023
概括
这项研究介绍了一种用于光子量子模拟器的新门电路,将单光子雪崩二极管 (SPAD) 集成到芯片上. 该电路表现出快速响应时间和高光子检测概率,这对于量子计算进步至关重要.
科学领域:
- 量子计算是一种量子计算.
- 综合光子学 综合光子学
- 半导体设备物理学 半导体设备物理
背景情况:
- 光子量子模拟器需要精确控制光子检测.
- 集成的单光子雪崩二极管 (SPAD) 是灵敏光检测的关键组件.
- 现有的封闭电路可能缺乏先进量子应用所需的速度和集成.
研究的目的:
- 介绍和描述用于光子量子模拟器的新型单体门电路.
- 为了评估在开发的网关电路中集成的SPAD的性能.
- 为了证明电路在高保真度量子信息处理方面的潜力.
主要方法:
- 采用0.18微米高压CMOS技术实现一个九通道门电路的单体实现.
- 在特定应用集成电路 (ASIC) 中集成九个SPAD.
- 电路参数的表征,包括升降时间,脉冲宽度,检测值和功耗.
主要成果:
- 实现了480 ps和280 ps的快速上升和下降时间,最小脉冲宽度为1.26 ns.
- 使用快速比较器启用了雪崩事件 (<100 mV) 的低检测值.
- 证明光子检测概率在9.9V过量偏差和635nm波长下为50%左右.
- 九个频道的总功耗约为250mW.
结论:
- 开发的封闭电路提供了适合光子量子模拟的高性能指标.
- 集成的SPAD对量子应用具有有前途的特性.
- 这种基于ASIC的解决方案推动了紧和高效的量子计算硬件的开发.
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