2014 15th International Radar Symposium (IRS) 2014
DOI: 10.1109/irs.2014.6869256
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Time-frequency transform used in radar Doppler tomography

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Cited by 5 publications
(5 citation statements)
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“…The frequency information related to time cannot be obtained by Fourier method, so it is not the mainstream method of micro-Doppler features extraction. For timefrequency analysis, the main methods include short-time Fourier transform [38], generalized S-transform [39], Gabor transform [40]- [42] and so on. Gabor transform is a short-time Fourier transform with Gaussian window.…”
Section: Radar Decision Processingmentioning
confidence: 99%
“…The frequency information related to time cannot be obtained by Fourier method, so it is not the mainstream method of micro-Doppler features extraction. For timefrequency analysis, the main methods include short-time Fourier transform [38], generalized S-transform [39], Gabor transform [40]- [42] and so on. Gabor transform is a short-time Fourier transform with Gaussian window.…”
Section: Radar Decision Processingmentioning
confidence: 99%
“…e frequency information related to the time cannot be obtained by the Fourier method, so it is not the mainstream method of micro-Doppler feature extraction. For time-frequency analysis, the main methods include shorttime Fourier transform [39], generalized S-transform [40], and Gabor transform [41][42][43]. Gabor transform is a shorttime Fourier transform with a Gaussian window.…”
Section: Radar Decision Processing Chenmentioning
confidence: 99%
“…1 to describe line integrals and projections. A one‐dimensional (1D) projection P θ ( r ) at angle θ is defined as the Radon transform of a two‐dimensional (2D) target function f ( x , y ) [20, 21]Pθfalse(rfalse)=normal∞normal∞thinmathspaceffalse(x,yfalse)δfalse(rxcosθysinθfalse)thinmathspacenormaldxthinmathspacenormaldy, where r is the distance from origin to the integral line.…”
Section: Foundations Of M–d Imaging and Simulations Studymentioning
confidence: 99%
“…The core idea of tomographic reconstruction is the Fourier slice theorem [20, 21]. The theorem states that the 1D Fourier transform of a parallel projection at a specific angle θ is equal to a slice of the 2D Fourier transform of the original target at the same angle, that isSθ)(kr=normal∞+normal∞Pθ(r)exp)(jkrrthinmathspacenormaldr=Fθ)(kx,ky. Where k x = k r cos θ , k y = k r sin θ are the spatial frequency components; F θ ( k x , k y ) is a slice of the 2D Fourier transform of the function f ( x , y ) along the direction of θ .…”
Section: Foundations Of M–d Imaging and Simulations Studymentioning
confidence: 99%
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