Optimal apodization design for medical ultrasound using constrained least squares part II simulation results

For Part I see ibid., vol. 54, p. 332-342 (2007). In the first part of this work, we introduced a novel general ultrasound apodization design method using constrained least squares (CLS). The technique allows for the design of system spatial impulse responses with narrow mainlobes and low sidelobes. In the linear constrained least squares (LCLS) formulation, the energy of the point spread function (PSF) outside a certain mainlobe boundary was minimized while maintaining a peak gain at the focus. In the quadratic constrained least squares (QCLS) formulation, the energy of the PSF outside a certain boundary was minimized, and the energy of the PSF inside the boundary was held constant. In this paper, we present simulation results that demonstrate the application of the CLS methods to obtain optimal system responses. We investigate the stability of the CLS apodization design methods with respect to errors in the assumed wave propagation speed. We also present simulation results that implement the CLS design techniques to improve cystic resolution. According to novel performance metrics, our apodization profiles improve cystic resolution by 3 dB to 10 dB over conventional apodizations such as the Hat, Hamming, and Nuttall windows. We also show results using the CLS techniques to improve conventional depth of field (DOF)

[1]  A. Nuttall Some windows with very good sidelobe behavior , 1981 .

[2]  G E Trahey,et al.  The impact of sound speed errors on medical ultrasound imaging. , 2000, The Journal of the Acoustical Society of America.

[3]  Marc Moonen,et al.  Design of far-field and near-field broadband beamformers using eigenfilters , 2003, Signal Process..

[4]  S. W. Smith,et al.  A contrast-detail analysis of diagnostic ultrasound imaging. , 1982, Medical physics.

[5]  R. F. Wagner,et al.  Low Contrast Detectability and Contrast/Detail Analysis in Medical Ultrasound , 1983, IEEE Transactions on Sonics and Ultrasonics.

[6]  W.F. Walker,et al.  A spline-based approach for computing spatial impulse responses , 2007, IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control.

[7]  C. Sidney Burrus,et al.  Constrained least square design of FIR filters without specified transition bands , 1996, IEEE Trans. Signal Process..

[8]  Gordon S. Kino,et al.  A theory for the radiation pattern of a narrow‐strip acoustic transducer , 1980 .

[9]  J. Goodman Introduction to Fourier optics , 1969 .

[10]  M. E. Anderson,et al.  Spatial quadrature: a novel technique for multi-dimensional velocity estimation , 1997, 1997 IEEE Ultrasonics Symposium Proceedings. An International Symposium (Cat. No.97CH36118).

[11]  W. Gander Least squares with a quadratic constraint , 1980 .

[12]  W.F. Walker,et al.  The application of k-space in pulse echo ultrasound , 1998, IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control.

[13]  J. Jensen,et al.  A new method for estimation of velocity vectors , 1998, IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control.

[14]  W. Walker,et al.  A fundamental limit on delay estimation using partially correlated speckle signals , 1995, IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control.

[15]  Chi-Wah Kok,et al.  Constrained eigenfilter design without specified transition bands , 2004, 2004 IEEE International Conference on Acoustics, Speech, and Signal Processing.

[16]  J. Bushberg The Essential Physics of Medical Imaging , 2001 .

[17]  W.F. Walker,et al.  Optimal apodization design for medical ultrasound using constrained least squares part I: theory , 2007, IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control.

[18]  S. Pei,et al.  2-D FIR eigenfilters: a least-squares approach , 1990 .

[19]  C.A. Cain,et al.  Multiple-focus ultrasound phased-array pattern synthesis: optimal driving-signal distributions for hyperthermia , 1989, IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control.