Abstract

In continuous-wave (CW) radar systems, such as frequency-modulated (FMCW), frequency-stepped (FSCW), or orthogonal frequency-division multiplexing (OFDM) radar systems, the range and velocity uncertainty are significantly impaired by phase noise decorrelation. Therefore, radar designers require accurate knowledge of their synthesizers’ phase noise profiles to assess and predict radar performance. However, commercial phase noise analyzers cannot determine phase noise during modulation, and this may differ notably from phase noise in the pure CW mode. Recent methods for FMCW phase noise analysis usually require comprehensive <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${a}$ </tex-math></inline-formula> <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">priori</i> knowledge of modulation parameter and are prone to systematic deviations. To overcome these issues, we propose a new approach based on differential analysis of subsequent time-domain measurements. This method retains, statistical phase noise information while reducing systematic influences. For the first time, less <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${a}$ </tex-math></inline-formula> <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">priori</i> signal knowledge is required, and the method works for nearly any kind of broadband signal modulation. The concept requires only a digitizer (e.g., an oscilloscope) and some digital signal processing. The proposed method is first experimentally tested with different phase-locked-loop (PLL)-based synthesizer phase noise profiles. The obtained phase noise profiles agree perfectly with the results of an established measurement system. After this proof of basic functionality, the unique phase noise analysis capability for BB modulated signals is demonstrated with PLL-generated FMCW signals. The results reveal a significant phase noise difference between the different setups and clearly show the capability and benefit of the novel phase noise spectral density measurement concept.

Highlights

  • I N THE field of commercial radar technology broadband continuous-wave (CW) radar systems, such as frequency-modulated (FMCW), frequency-stepped (FSCW), or orthogonal frequency-division

  • In the case of long-range measurements, phase noise leads to a reduction in the target signal power spectral density (PSD) and a notably reduced signal-to-noise ratio (SNR) in the beat spectra

  • The method is most suitable for cases where the modulation parameters are invariant from realization to realization

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Summary

INTRODUCTION

I N THE field of commercial radar technology (e.g., automotive, industrial, or aerospace) broadband continuous-wave (CW) radar systems, such as frequency-modulated (FMCW), frequency-stepped (FSCW), or orthogonal frequency-division. Some, such as spectrum analyzers, use direct methods, whereas signal source analyzers use techniques with phase detectors or two-channel cross correlation These methods differ in terms of their sensitivity and dynamics, but they are all limited to measuring the phase noise of mono-frequency sinusoidal signals. The simplest way to measure the change in phase noise when operating a PLL in the FMCW mode was to measure it in the feedback path of the PLL in front of the phase detector This was done by exploiting the fact that the feedback signal at the phase detector is available as a mono-frequency sinusoidal signal that can be measured directly with a commercial phase noise measurement device.

PHASE NOISE MEASUREMENT OF FMCW CHIRPS
Theory and Classical Approach
Proposed Approach
EXPERIMENTAL VERIFICATION
Concept and Setup for Experimental Verification
PHASE NOISE MEASUREMENT OF FMCW CHIRP
Scenario 1
Measurement Setup
Results
CONCLUSION
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