用于磁感应的带脉冲整形 FIR DAC 的小面积无二阶加法连续时间 ΔΣ 调制器

IF 2.4 Q2 ENGINEERING, ELECTRICAL & ELECTRONIC
Manish Srivastava;Alessandro Ferro;Aleksandr Sidun;José M. De La Rosa;Kilian O’Donoghue;Pádraig Cantillon-Murphy;Daniel O’Hare
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引用次数: 0

摘要

本研究提出了一种小面积二阶连续时间ΔΣ调制器(CT $\Delta \Sigma \text{M}$),它采用单个低压差稳压器(LDO)作为 CT $\Delta \Sigma \text{M}$的电源和参考电压缓冲器。CT $\Delta \Sigma \text{M}$用于对图像引导和机器人手术的磁跟踪等应用中的极低振幅信号进行数字化。为了最大限度地减少硅片面积,我们提出了一种采用无加法器架构的前馈架构级联积分器。此外,还提出了一种新型连续时间脉冲型数模转换器(CT-PS DAC),用于过量环路延迟(ELD)补偿,以简化基准电压缓冲器的电流驱动要求。这样,单个低压差 (LDO) 稳压器就能为 DAC 提供电源和 $\text{V}_{ref}$。该电路采用 65-nm CMOS 技术设计,在 20 kHz 信号带宽内实现了 82-dB SNDR 峰值和 91-dB DR 峰值,当时钟频率为 10.24 MHz 时,CT $\Delta \Sigma \text{M}$ 的功耗为 300 ~\mu \text{W}$。CT $\Delta \Sigma \text{M}$ 的最新面积为 0.07 mm2。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
A Small-Area 2nd-Order Adder-Less Continuous-Time ΔΣ Modulator With Pulse Shaping FIR DAC for Magnetic Sensing
This work presents a small-area 2nd-order continuous-time $\Delta \Sigma $ Modulator (CT $\Delta \Sigma \text{M}$ ) with a single low dropout regulator (LDO) serving as both the power supply for the CT $\Delta \Sigma \text{M}$ and reference voltage buffer. The CT $\Delta \Sigma \text{M}$ is used for digitising very low amplitude signals in applications such as magnetic tracking for image-guided and robotic surgery. A cascade of integrators in a feed-forward architecture implemented with an adder-less architecture has been proposed to minimise the silicon area. In addition, a novel continuous-time pulse-shaped digital-to-analog converter (CT-PS DAC) is proposed for excess loop delay (ELD) compensation to simplify the current drive requirements of the reference voltage buffer. This enables a single low-dropout (LDO) voltage regulator to generate both power supply and $\text{V}_{ref}$ for the DAC. The circuit has been designed in 65-nm CMOS technology, achieving a peak 82-dB SNDR and 91-dB DR within a signal bandwidth of 20 kHz and the CT $\Delta \Sigma \text{M}$ consumes $300 ~\mu \text{W}$ of power when clocked at 10.24 MHz. The CT $\Delta \Sigma \text{M}$ achieves a state-of-the-art area of 0.07 mm2.
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