Gary C. Ng
Philips
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Featured researches published by Gary C. Ng.
IEEE Transactions on Ultrasonics Ferroelectrics and Frequency Control | 2003
Russell J. Fedewa; Kirk D. Wallace; Mark R. Holland; James R. Jago; Gary C. Ng; Matthew R. Rielly; Brent S. Robinson; James G. Miller
Correlation-based approaches to phase aberration correction rely on the spatial coherence of backscattered signals. The spatial coherence of backscatter from speckle-producing targets is predicted by the auto correlation of the transmit apodization (Van Cittert-Zernike theorem). Work by others indicates that the second harmonic beam has a wider mainlobe with lower sidelobes than a beam transmitted at 2f. The purpose of this paper is to demonstrate that the spatial coherence of backscatter for the second harmonic is different from that of the fundamental, as would be anticipated from applying the Van Cittert-Zernike theorem to the reported measurements of the second harmonic field. Another objective of this work is to introduce the concept of the effective apodization and to verify that the effective apodization of the second harmonic is narrower than the transmit apodization. The spatial coherence of backscatter was measured using three clinical arrays with a modified clinical imaging system. The spatial coherence results were verified using a pseudo-array scan in a transverse plane of the transmitted field with a hydrophone. An effective apodization was determined by backpropagating these values using a linear angular spectrum approach. The spatial coherence for the harmonic portion of backscatter differed systematically and significantly from the auto correlation of the transmit apodization.
IEEE Transactions on Ultrasonics Ferroelectrics and Frequency Control | 2004
Russell J. Fedewa; Kirk D. Wallace; Mark R. Holland; James R. Jago; Gary C. Ng; Matthew R. Rielly; Brent S. Robinson; James G. Miller
To be successful, correlation-based, phase-aberration correction requires a high correlation among backscattered signals. For harmonic imaging, the spatial coherence of backscatter for the second harmonic component is different than the spatial coherence of backscatter for the fundamental component. The purpose of this work was to determine the effect of changing the transmit apodization on the spatial coherence of backscatter for the nonlinearly generated second harmonic. Our approach was to determine the effective apodizations for the fundamental and second harmonic using both experimental measurements and simulations. Two-dimensional measurements of the transverse cross sections of the finite-amplitude ultrasonic fields generated by rectangular and circular apertures were acquired with a hydrophone. Three different one-dimensional transmit apodization functions were investigated: uniform, Riesz, and trapezoidal. An effective apodization was obtained for each transmit apodization by backpropagating the values measured from within the transmit focal zone using a linear angular spectrum approach. Predictions of the spatial coherence of backscatter were obtained using the pulse-echo Van Cittert-Zernike theorem. In all cases the effective apodization at 2f was narrower than the transmit apodization. We demonstrate that certain transmit apodizations result in a greater spatial coherence of backscatter at the second harmonic than at the fundamental.
internaltional ultrasonics symposium | 2002
Russell J. Fedewa; Kirk D. Wallace; Mark R. Holland; James R. Jago; Gary C. Ng; Matthew R. Rielly; Brent S. Robinson; James G. Miller
The present work measures the effective apodizations for the fundamental and second harmonic and uses the Van Cittert-Zernike theorem to predict the spatial coherence of the second harmonic portion of backscatter. Two-dimensional pseudo-array scans of a transverse cross section of the finite amplitude ultrasonic fields generated by rectangular and circular apertures were performed with a hydrophone. Three transmit apodization functions were investigated: rectangular, Riesz, and trapezoidal. An effective apodization was obtained by backpropagating the values measured from within the transmit focal zone using a linear angular spectrum approach. In all cases the effective apodization at 2f was narrower than the transmit apodization. Our results demonstrate that choices of apodization can be identified that yield better spatial coherence at the second harmonic than at the fundamental.
computer assisted radiology and surgery | 2016
Parmida Beigi; Robert Rohling; Septimiu E. Salcudean; Gary C. Ng
PurposeThis paper presents a new approach to detect a standard handheld needle in ultrasound-guided interventions.MethodsOur proposal is to use natural hand tremor, which causes minute displacement of the needle, to detect the needle in ultrasound B-mode images. Subtle displacements arising from tremor motion have a periodic pattern which is usually imperceptible to the naked eye in the B-mode image. We use these displacement measurements in a spatiotemporal framework to detect linear structures with periodic pattern among a sequence of frames. The needle trajectory is estimated as a linear path in the image having maximum spectral correlation with the time trace of displacement due to tremor. A coarse estimation process is followed by a fine estimation step, where the motion pattern is analyzed along spatiotemporal linear paths with various angles originating from the estimated puncture site, within the trajectory channel. Spectral coherency is derived for each sample path versus the reference path, and the needle trajectory is identified as the mean of the sample paths with the maximum coherence within the tremor frequency range.ResultsTo evaluate the detection accuracy, we tested the method in vivo on porcine tissue, where the needle was inserted into the biceps femoris muscle. To understand whether tremor itself affects needle position, the maximum angular change due to tremor was calculated: mean, standard deviation (SD) and root-mean-square (RMS) measurement of
internaltional ultrasonics symposium | 2001
Russell J. Fedewa; Kirk D. Wallace; Mark R. Holland; James R. Jago; Gary C. Ng; Matthew R. Rielly; Brent S. Robinson; James G. Miller
IEEE Transactions on Medical Imaging | 2017
Arash Pourtaherian; Harm J. Scholten; Lieneke Kusters; S Sveta Zinger; Nenad Mihajlovic; Alexander Franciscus Kolen; Fei Zuo; Gary C. Ng; H.H.M. Korsten
0.43^\circ , 0.23^\circ
Ultrasonics | 2017
Parmida Beigi; Robert Rohling; Tim Salcudean; Victoria A. Lessoway; Gary C. Ng
internaltional ultrasonics symposium | 2016
Arash Pourtaherian; Nenad Mihajlovic; S Sveta Zinger; H.H.M. Korsten; Jinfeng Huang; Gary C. Ng
0.43∘,0.23∘ and
medical image computing and computer assisted intervention | 2017
Arash Pourtaherian; Farhad Ghazvinian Zanjani; S Sveta Zinger; Nenad Mihajlovic; Gary C. Ng; H.H.M. Korsten
Medical Imaging 2018: Image-Guided Procedures, Robotic Interventions, and Modeling | 2018
Farhad Ghazvinian Zanjani; Arash Pourtaherian; Xikai Tang; Svitlana Zinger; Nenad Mihajlovic; Gary C. Ng; H.H.M. Korsten
0.48^\circ