2014 International Radar Conference 2014
DOI: 10.1109/radar.2014.7060365
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2D indoor localization system using FMCW radars and DMTD technique

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Cited by 8 publications
(5 citation statements)
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“…In recent years, with the continuous development of antenna technology and integrated circuits, K‐band millimeter wave radar systems have been widely used in human body monitoring, 1,2 automotive sensing, 3,4 indoor localization, 5 and other fields. As the front end of the radar system, the antenna needs to transmit and receive electromagnetic waves, so the design of the antenna directly affects the performance of the system.…”
Section: Introductionmentioning
confidence: 99%
“…In recent years, with the continuous development of antenna technology and integrated circuits, K‐band millimeter wave radar systems have been widely used in human body monitoring, 1,2 automotive sensing, 3,4 indoor localization, 5 and other fields. As the front end of the radar system, the antenna needs to transmit and receive electromagnetic waves, so the design of the antenna directly affects the performance of the system.…”
Section: Introductionmentioning
confidence: 99%
“…Other UWB navigation solutions with the known position of transmitters are presented in Tiemann and Wietfeld [7], Kaniewski et al [8] and Krishnan et al [9]. It is also worth noting that in Kumar et al [10] a bistatic frequency modulated continuous wave (FMCW) radar is used to localise the active tags indoors. All these methods rely on knowledge of the position of transmitters.…”
Section: Introductionmentioning
confidence: 99%
“…Meanwhile, by adjusting the values of the TTDs, we can let the beamforming at the M -th subcarrier f M point to an end angle θ end . Specifically, we set 12), and derive…”
Section: B Utilizing the Beam Squint For Sensingmentioning
confidence: 99%
“…Afterward, the beams from the 0-th subcarrier to the M -th subcarrier will gradually squint from the start angle θ start to the end angle θ end in a controlled way. For subcarrier f m , its beamforming angle θ m still satisfies (12) and can be computed as follows. Substitute θ = θ m ,…”
Section: B Utilizing the Beam Squint For Sensingmentioning
confidence: 99%
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