Side Lobe Reduction Using Centroid and Flatness in Passive Cavitation Imaging

M. Jeong, Sung Jae Kwon, M. Choi
{"title":"Side Lobe Reduction Using Centroid and Flatness in Passive Cavitation Imaging","authors":"M. Jeong, Sung Jae Kwon, M. Choi","doi":"10.1109/ULTSYM.2019.8925582","DOIUrl":null,"url":null,"abstract":"Cavitation bubbles generated by high-intensity focused ultrasound strongly collapse and emit ultrasound waves. Since passive cavitation imaging can be performed using only receive focusing, side lobes appear over a wide area of an image. The delay and sum beamforming technique used to construct passive cavitation images cannot effectively image the cavitation occurrence time and spatial distribution because a small cavitation signal is buried in the side lobe of a large cavitation signal when there are a large number of cavitation bubbles. The ultrasound wave emitted when the cavitation bubble collapses is a short duration pulse. After compensating for the focusing delay, the signals due to the main lobe (at the imaging point) received at each element of the transducer array are similar in magnitude, but those due to the side lobes (other than the imaging point) is significant only at some elements of the array. Using this characteristic of the received channel data, we propose both centroid and flatness as metrics to evaluate the effect of the main and side lobes at imaging points. If the centroid of the signal magnitude distribution of the entire receiving channel is positioned at the center of the array, the signal is considered to be due to the main lobe. However, if the centroid is computed to be located near both ends of the array, the signal is considered to be due to the side lobes. If the signals are found to be due to the side lobes in passive cavitation imaging, the pixel brightness is reduced by weighting using the centroid and flatness metrics. We computed the centroid and flatness metrics using computer simulation and experimental data, and confirmed the suppression of side lobes by multiplying the image by a weight using the centroid and flatness. The proposed method makes it easier to observe cavitation by effectively removing side lobes from passive cavitation images when the number of cavitation bubbles is not large.","PeriodicalId":6759,"journal":{"name":"2019 IEEE International Ultrasonics Symposium (IUS)","volume":"28 1","pages":"1455-1458"},"PeriodicalIF":0.0000,"publicationDate":"2019-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2019 IEEE International Ultrasonics Symposium (IUS)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ULTSYM.2019.8925582","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0

Abstract

Cavitation bubbles generated by high-intensity focused ultrasound strongly collapse and emit ultrasound waves. Since passive cavitation imaging can be performed using only receive focusing, side lobes appear over a wide area of an image. The delay and sum beamforming technique used to construct passive cavitation images cannot effectively image the cavitation occurrence time and spatial distribution because a small cavitation signal is buried in the side lobe of a large cavitation signal when there are a large number of cavitation bubbles. The ultrasound wave emitted when the cavitation bubble collapses is a short duration pulse. After compensating for the focusing delay, the signals due to the main lobe (at the imaging point) received at each element of the transducer array are similar in magnitude, but those due to the side lobes (other than the imaging point) is significant only at some elements of the array. Using this characteristic of the received channel data, we propose both centroid and flatness as metrics to evaluate the effect of the main and side lobes at imaging points. If the centroid of the signal magnitude distribution of the entire receiving channel is positioned at the center of the array, the signal is considered to be due to the main lobe. However, if the centroid is computed to be located near both ends of the array, the signal is considered to be due to the side lobes. If the signals are found to be due to the side lobes in passive cavitation imaging, the pixel brightness is reduced by weighting using the centroid and flatness metrics. We computed the centroid and flatness metrics using computer simulation and experimental data, and confirmed the suppression of side lobes by multiplying the image by a weight using the centroid and flatness. The proposed method makes it easier to observe cavitation by effectively removing side lobes from passive cavitation images when the number of cavitation bubbles is not large.
被动空化成像中利用质心和平整度减少旁瓣
高强度聚焦超声产生的空化气泡强烈坍缩并发射超声波。由于被动空化成像可以只使用接收聚焦,侧瓣出现在图像的广泛区域。利用延时和和波束形成技术构建被动空化图像,由于存在大量空化泡时,小的空化信号被埋在大的空化信号的旁瓣中,无法有效成像空化发生的时间和空间分布。空化泡破裂时发出的超声波为短脉冲。补偿聚焦延迟后,换能器阵列各单元接收到的主瓣(成像点)信号大小相近,而副瓣(成像点以外)信号仅在阵列的某些单元显著。利用接收通道数据的这一特性,我们提出了质心和平坦度作为度量来评估成像点的主瓣和副瓣的影响。如果整个接收信道的信号幅度分布的质心位于阵列的中心,则认为该信号是由于主瓣。但是,如果计算质心位于阵列的两端附近,则认为信号是由侧瓣引起的。如果在被动空化成像中发现信号是由于侧瓣引起的,则通过使用质心和光度度量加权来降低像素亮度。我们利用计算机模拟和实验数据计算了质心和平面度量,并通过将图像乘以使用质心和平面度的权值来证实对侧瓣的抑制。该方法在空化气泡数量不大的情况下,通过有效地去除被动空化图像中的侧瓣,使空化现象的观察更加容易。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 求助全文
来源期刊
自引率
0.00%
发文量
0
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术官方微信