Abstract

The calibration of correlation radiometers, and particularly aperture synthesis interferometric radiometers, is a critical issue to ensure their performance. Current calibration techniques are based on the measurement of the cross-correlation of receivers’ outputs when injecting noise from a common noise source requiring a very stable distribution network. For large interferometric radiometers this centralized noise injection approach is very complex from the point of view of mass, volume and phase/amplitude equalization. Distributed noise injection techniques have been proposed as a feasible alternative, but are unable to correct for the so-called “baseline errors” associated with the particular pair of receivers forming the baseline. In this work it is proposed the use of centralized Pseudo-Random Noise (PRN) signals to calibrate correlation radiometers. PRNs are sequences of symbols with a long repetition period that have a flat spectrum over a bandwidth which is determined by the symbol rate. Since their spectrum resembles that of thermal noise, they can be used to calibrate correlation radiometers. At the same time, since these sequences are deterministic, new calibration schemes can be envisaged, such as the correlation of each receiver’s output with a baseband local replica of the PRN sequence, as well as new distribution schemes of calibration signals. This work analyzes the general requirements and performance of using PRN sequences for the calibration of microwave correlation radiometers, and particularizes the study to a potential implementation in a large aperture synthesis radiometer using an optical distribution network.

Highlights

  • Synthetic aperture interferometric radiometers have been successfully used in radio-astronomy and more recently, they have been proposed for Earth observation as well

  • Two calibration methods are considered: injecting noise [Fringe-Wash Function (FWF)(noise)], as in Figure 1a with the switch in position 1, and injecting the Pseudo-Random Noise (PRN) sequence [FWF(Y1·Y2)], as in Figure 1a with the switch in position 2. In both the cases several noise sources affect the result of Equation (1) such as the noise distribution network, the thermal noise present in PRN signal itself, leakages of the local oscillator noise through the mixer etc

  • 3). b) FWF estimated by cross-correlating receivers’ outputs when calibration signal is a PRN sequence FWF(Y1·Y2) (Equations 1-2) for different number of quantization bits and comparison with reference FWF computed with correlated noise with the one injected (TN) = 1500 K

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Summary

Introduction

Synthetic aperture interferometric radiometers have been successfully used in radio-astronomy and more recently, they have been proposed for Earth observation as well. The calibration of microwave correlation radiometers (either aperture synthesis, interferometric, or polarimetric) can benefit from these properties by replacing the noise sources by PRN generators This approach has several advantages: the signal amplitude is constant, which allows higher receivers input power levels than in the case of injecting noise, without the need to allow a margin to avoid signal clipping. A summary of the main conclusions of this work are discussed This innovative technique for calibrating microwave correlation radiometers can be applied as well to other communication systems or phased-arrays where the receiver’s frequency response needs to be measured with the system turned on

Theoretical Basis and Simulator Description
Experimental Validation of the Technique
Findings
Conclusions
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