1992
DOI: 10.1109/36.158868
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The theory and mechanical realization of an ideal scanning method for a single-channel imaging microwave radiometer

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Cited by 13 publications
(3 citation statements)
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“…Since the T B of the target depends, in addition to frequency and polarization, on the incidence angle ψ, in the conical scanning each pixel in a single sweep (or scan) is observed at the same ψ [9,10]. To produce an image of the scenario, we have to change the value of ψ at each sweep.…”
Section: Conical Scanningmentioning
confidence: 99%
“…Since the T B of the target depends, in addition to frequency and polarization, on the incidence angle ψ, in the conical scanning each pixel in a single sweep (or scan) is observed at the same ψ [9,10]. To produce an image of the scenario, we have to change the value of ψ at each sweep.…”
Section: Conical Scanningmentioning
confidence: 99%
“…Figure 4 shows the scan parameters, scan patterns, the resulting images and data cross-sections of the ideal parallel scan for the HUT 93 GHz imager (Kemppinen and Hallikainen, 1992), modified TUDRAD (Skou, 1978) and a pendulum scan, for which the time spent on sampling is maximized, leading to heavy alongtrack oversampling. The platform is assumed stable in each case.…”
Section: Simulation Resultsmentioning
confidence: 99%
“…Previously, we presented a mathematical model for conical scan pattern optimization (Kemppinen and Hallikainen, 1992), but had no tool for comparing its performance with traditional patterns. At present, we are building a versatile 93 GHz imaging radiometer being capable of the comparison.…”
Section: Introductionmentioning
confidence: 99%