TY - GEN
T1 - Ultrasound harmonic imaging using nonlinear chirp for cardiac imaging
AU - Song, Hyun Jae
AU - Song, Jaehee
AU - Chang, Jin Ho
AU - Song, Tai Kyong
PY - 2010
Y1 - 2010
N2 - Coded excitation techniques have been used to improve a signal-to-noiseratio (SNR) in tissue harmonic imaging. However, a poor separation betweenfundamental and target harmonic components causes the second harmonic signals tohave a high level of range sidelobes after compression. In terms of theseparation performance, pulse inversion (PI) is the best method and thusprovides the lowest level of range sidelobes compared to bandpass filtering(BPF) and power modulation. However, the PI requires two transmit steps, thusinevitably decreasing frame rate. This paper proposes a new coded excitationtechnique using a nonlinear chirp for tissue harmonic imaging, particularlycardiac imaging. Since the spectral overlap between a transmitted nonlinearchirp and its second harmonic counterpart is less than the case of linear chirp,a simple BPF can be used for the separation so as to provide the range sidelobelevels comparable to those produced by PI without a loss of frame rate. In theexperiments, the highest level of the sidelobes of the nonlinear chirp was 40.59dB, which was comparable to the value from PI, i.e., 39.84 dB.
AB - Coded excitation techniques have been used to improve a signal-to-noiseratio (SNR) in tissue harmonic imaging. However, a poor separation betweenfundamental and target harmonic components causes the second harmonic signals tohave a high level of range sidelobes after compression. In terms of theseparation performance, pulse inversion (PI) is the best method and thusprovides the lowest level of range sidelobes compared to bandpass filtering(BPF) and power modulation. However, the PI requires two transmit steps, thusinevitably decreasing frame rate. This paper proposes a new coded excitationtechnique using a nonlinear chirp for tissue harmonic imaging, particularlycardiac imaging. Since the spectral overlap between a transmitted nonlinearchirp and its second harmonic counterpart is less than the case of linear chirp,a simple BPF can be used for the separation so as to provide the range sidelobelevels comparable to those produced by PI without a loss of frame rate. In theexperiments, the highest level of the sidelobes of the nonlinear chirp was 40.59dB, which was comparable to the value from PI, i.e., 39.84 dB.
KW - Harmonic imaging
KW - Nonlinear chirp
KW - Spectral overlap
KW - coded excitation
UR - https://www.scopus.com/pages/publications/80054083920
U2 - 10.1109/ULTSYM.2010.5935659
DO - 10.1109/ULTSYM.2010.5935659
M3 - Conference contribution
AN - SCOPUS:80054083920
SN - 9781457703829
T3 - Proceedings - IEEE Ultrasonics Symposium
SP - 2008
EP - 2011
BT - 2010 IEEE International Ultrasonics Symposium, IUS 2010
T2 - 2010 IEEE International Ultrasonics Symposium, IUS 2010
Y2 - 11 October 2010 through 14 October 2010
ER -