1988
DOI: 10.1109/8.1177
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Error analysis techniques for planar near-field measurements

Abstract: Abstract-The results of an extensive error analysis on planar nearfield measurements are described. The analysis provides ways for estimating the magnitude of each individual source of error and then combining them to estimate the total uncertainty in the measurement. Mathematical analysis, computer simulation, and measurement tests are all used where appropriate.

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Cited by 260 publications
(149 citation statements)
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“…λ/2 sample spacing is commonly adopted along the length of the cylinder in the standard cylindrical and in the planar measurements due to FFT usage. Sample spacings coarser than λ/2 result in aliasing errors [5]. However, no such limitation applies to FIAFTA and the sample spacing is computed in relation with the number of unknowns required to solve the linear system of equations.…”
Section: Data Point Spacingmentioning
confidence: 99%
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“…λ/2 sample spacing is commonly adopted along the length of the cylinder in the standard cylindrical and in the planar measurements due to FFT usage. Sample spacings coarser than λ/2 result in aliasing errors [5]. However, no such limitation applies to FIAFTA and the sample spacing is computed in relation with the number of unknowns required to solve the linear system of equations.…”
Section: Data Point Spacingmentioning
confidence: 99%
“…Therefore, the resulting error estimates predict an error which is unrealistically high. Newell performed more realistic error analyses in [5] making use of a known spatial dependency of the errors. This comprehensive analysis identifies the significant errors and also estimates the magnitude of all near-field error sources.…”
Section: Introductionmentioning
confidence: 99%
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“…Special attention must be given to the probe pattern and positioning accuracy [1] as well as to the effects that error sources in NF acquisitions, such as truncation of the measurement plane, cable flexing, stray signals, leakage, etc., can introduce in the FF pattern of the AUT [1,2,13,14]. 1 The far-field distance is defined by R ¼ 2D 2 =λ (R >> λ), being D the maximum dimension of the antenna and λ the wavelength [1].…”
Section: Introductionmentioning
confidence: 99%
“…Nevertheless, phase acquisition, particularly at mm-and submm-wave bands, is a challenging task that requires sophisticated and expensive equipment due to the high thermal stability requirements and the effect of the errors, mostly resulting from thermal drift and cable flexing [1,[13][14][15][16].…”
Section: Introductionmentioning
confidence: 99%