7.4 A 915MHz asymmetric radio using Q-enhanced amplifier for a fully integrated 3×3×3mm3 wireless sensor node with 20m non-line-of-sight communication

Li-Xuan Chuo, Yao Shi, Zhihong Luo, N. Chiotellis, Z. Foo, Gyouho Kim, Yejoong Kim, A. Grbic, D. Wentzloff, Hun-Seok Kim, D. Blaauw
{"title":"7.4 A 915MHz asymmetric radio using Q-enhanced amplifier for a fully integrated 3×3×3mm3 wireless sensor node with 20m non-line-of-sight communication","authors":"Li-Xuan Chuo, Yao Shi, Zhihong Luo, N. Chiotellis, Z. Foo, Gyouho Kim, Yejoong Kim, A. Grbic, D. Wentzloff, Hun-Seok Kim, D. Blaauw","doi":"10.1109/ISSCC.2017.7870296","DOIUrl":null,"url":null,"abstract":"Enabling long range (>10m) wireless communication in non-line-of sight (NLOS) scenarios would dramatically expand the application space and usability of mm-scale wireless sensor nodes. The major technical challenges posed by a mm-scale form-factor are poor antenna efficiency and the small instantaneous current limit (∼10s of μA) of thin-film batteries. We address these challenges in several ways: 1) We found that a magnetic dipole antenna achieves better efficiency at an electrically-small size than an electric dipole, when the antennas are resonated with off-chip lumped components. In addition, the high impedance of electrically-small electric dipoles (∼4kΩ compared to 10Ω for the magnetic antenna) requires an impractically large off-chip inductor to resonate. 2) By simultaneously considering the magnetic dipole efficiency, frequency-dependent path-loss, and wall penetration loss, we found that a 915MHz carrier frequency is optimal for a 3×3×3mm3 sensor node in NLOS asymmetric communication with a gateway. This is despite the resulting low antenna efficiency (0.21%) which typically drives mm-scale radios to operate at ≫1GHz frequency [1]. 3) In transmit (TX) mode, instead of using a PA and PLL, we utilize a cross-coupled driver to resonate the magnetic antenna at 915MHz with a quality factor (Q) of 110 in order to reduce overall power consumption. 4) In receive (RX) mode, we propose an approach of reusing the cross-coupled driver in a non-oscillating mode to raise the Q of the resonant tank to 300, resulting in 49dB voltage gain at 43µW, thereby replacing a power-hungry LNA and bulky off-chip filter. 5) A sparse pulse-position modulation (PPM) combined with a sensor-initiation communication protocol [2] shifts the power-hungry calibration of frequency offset to the gateway, enabling crystal-free radio design. The complete radio, including the transceiver IC, a 3D antenna, off-chip capacitors, a processor, a power management unit (PMU) and memory, is integrated within a 3×3×3mm3 sensor node, demonstrating stand-alone bi-directional 20m NLOS wireless communication with variable data rates of 30b/s to 30.3kb/s for TX and 7.8kb/s to 62.5kb/s for RX. The transmitter generates −26.9 dBm equivalent isotropically radiated power (EIRP) consuming 2mW power and the receiver has a sensitivity of −93dBm consuming 1.85mW.","PeriodicalId":269679,"journal":{"name":"2017 IEEE International Solid-State Circuits Conference (ISSCC)","volume":"35 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2017-03-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"42","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2017 IEEE International Solid-State Circuits Conference (ISSCC)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ISSCC.2017.7870296","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 42

Abstract

Enabling long range (>10m) wireless communication in non-line-of sight (NLOS) scenarios would dramatically expand the application space and usability of mm-scale wireless sensor nodes. The major technical challenges posed by a mm-scale form-factor are poor antenna efficiency and the small instantaneous current limit (∼10s of μA) of thin-film batteries. We address these challenges in several ways: 1) We found that a magnetic dipole antenna achieves better efficiency at an electrically-small size than an electric dipole, when the antennas are resonated with off-chip lumped components. In addition, the high impedance of electrically-small electric dipoles (∼4kΩ compared to 10Ω for the magnetic antenna) requires an impractically large off-chip inductor to resonate. 2) By simultaneously considering the magnetic dipole efficiency, frequency-dependent path-loss, and wall penetration loss, we found that a 915MHz carrier frequency is optimal for a 3×3×3mm3 sensor node in NLOS asymmetric communication with a gateway. This is despite the resulting low antenna efficiency (0.21%) which typically drives mm-scale radios to operate at ≫1GHz frequency [1]. 3) In transmit (TX) mode, instead of using a PA and PLL, we utilize a cross-coupled driver to resonate the magnetic antenna at 915MHz with a quality factor (Q) of 110 in order to reduce overall power consumption. 4) In receive (RX) mode, we propose an approach of reusing the cross-coupled driver in a non-oscillating mode to raise the Q of the resonant tank to 300, resulting in 49dB voltage gain at 43µW, thereby replacing a power-hungry LNA and bulky off-chip filter. 5) A sparse pulse-position modulation (PPM) combined with a sensor-initiation communication protocol [2] shifts the power-hungry calibration of frequency offset to the gateway, enabling crystal-free radio design. The complete radio, including the transceiver IC, a 3D antenna, off-chip capacitors, a processor, a power management unit (PMU) and memory, is integrated within a 3×3×3mm3 sensor node, demonstrating stand-alone bi-directional 20m NLOS wireless communication with variable data rates of 30b/s to 30.3kb/s for TX and 7.8kb/s to 62.5kb/s for RX. The transmitter generates −26.9 dBm equivalent isotropically radiated power (EIRP) consuming 2mW power and the receiver has a sensitivity of −93dBm consuming 1.85mW.
7.4采用q增强放大器的915MHz非对称无线电,用于完全集成的3×3×3mm3无线传感器节点,具有20米非视距通信
在非视距(NLOS)场景下实现远距离(>10m)无线通信将极大地扩展毫米级无线传感器节点的应用空间和可用性。毫米尺寸带来的主要技术挑战是天线效率差和薄膜电池的瞬时电流限制(μA ~ 10s)小。我们以几种方式解决这些挑战:1)我们发现,当天线与片外集总元件共振时,磁偶极子天线在电小尺寸下比电偶极子天线获得更好的效率。此外,电小电偶极子的高阻抗(与磁天线的10Ω相比,约4kΩ)需要一个不切实际的大片外电感器来谐振。2)同时考虑磁偶极子效率、频率相关路径损耗和穿透壁损耗,发现在NLOS与网关的非对称通信中,3×3×3mm3传感器节点的最优载波频率为915MHz。尽管导致天线效率低(0.21%),这通常驱动毫米级无线电在1GHz频率上工作[1]。3)在发射(TX)模式下,我们使用交叉耦合驱动器来共振915MHz的磁天线,质量因子(Q)为110,而不是使用PA和PLL,以降低总体功耗。4)在接收(RX)模式下,我们提出了一种在非振荡模式下重用交叉耦合驱动器的方法,将谐振槽的Q提高到300,从而在43µW下获得49dB的电压增益,从而取代耗电的LNA和笨重的片外滤波器。5)稀疏脉冲位置调制(PPM)与传感器启动通信协议[2]相结合,将频率偏移的耗电校准转移到网关,从而实现无晶体无线电设计。完整的无线电,包括收发器IC、3D天线、片外电容器、处理器、电源管理单元(PMU)和存储器,集成在3×3×3mm3传感器节点中,演示了独立的双向20m NLOS无线通信,TX的可变数据速率为30b/s至30.3kb/s, RX的可变数据速率为7.8kb/s至62.5kb/s。发射器产生−26.9 dBm等效各向同性辐射功率(EIRP),消耗2mW功率,接收器的灵敏度为−93dBm,消耗1.85mW。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 求助全文
来源期刊
自引率
0.00%
发文量
0
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术官方微信