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Experimental and theoretical evaluation of microbubble behavior: effect of transmitted phase and bubble size.微泡行为的实验与理论评估:透射相位和气泡大小的影响
IEEE Trans Ultrason Ferroelectr Freq Control. 2000;47(6):1494-509. doi: 10.1109/58.883539.
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Optical and acoustical observations of the effects of ultrasound on contrast agents.超声对造影剂影响的光学与声学观察。
IEEE Trans Ultrason Ferroelectr Freq Control. 1999;46(1):220-32. doi: 10.1109/58.741536.
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Subharmonic response of encapsulated microbubbles: conditions for existence and amplification.包封微泡的亚谐波响应:存在与放大的条件
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Cavitation threshold of microbubbles in gel tunnels by focused ultrasound.聚焦超声作用下凝胶通道中微泡的空化阈值
Ultrasound Med Biol. 2007 Oct;33(10):1651-60. doi: 10.1016/j.ultrasmedbio.2007.04.018. Epub 2007 Jun 27.
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Role of acoustic cavitation in the delivery and monitoring of cancer treatment by high-intensity focused ultrasound (HIFU).声空化在高强度聚焦超声(HIFU)癌症治疗的递送与监测中的作用。
Int J Hyperthermia. 2007 Mar;23(2):105-20. doi: 10.1080/02656730701194131.
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Attenuation and size distribution measurements of Definity and manipulated Definity populations.Definity及处理后的Definity群体的衰减和尺寸分布测量
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7
Stable and transient subharmonic emissions from isolated contrast agent microbubbles.来自孤立的造影剂微泡的稳定和瞬态亚谐波发射。
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WFUMB Safety Symposium on Echo-Contrast Agents: nature and types of ultrasound contrast agents.WFUMB超声造影剂安全研讨会:超声造影剂的性质与类型
Ultrasound Med Biol. 2007 Feb;33(2):187-96. doi: 10.1016/j.ultrasmedbio.2006.07.008.
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Quantitative relations of acoustic inertial cavitation with sonoporation and cell viability.声学惯性空化与声孔效应及细胞活力的定量关系。
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包裹对比微泡的径向振动与后激发压力峰相关。

Encapsulated contrast microbubble radial oscillation associated with postexcitation pressure peaks.

机构信息

UPMC Univ Paris 06, UMR 7623, LIP, F-75005 Paris, France.

出版信息

J Acoust Soc Am. 2010 Feb;127(2):1156-64. doi: 10.1121/1.3277216.

DOI:10.1121/1.3277216
PMID:20136236
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC2852442/
Abstract

This work combines modeling and experiment to assess encapsulated microbubble oscillations associated with broadband pressure peaks detected after microbubble excitation (postexcitation signals). Data were acquired from albumin-shelled and phospholipid-shelled microbubbles using a passive cavitation detector consisting of a confocally aligned 2.8-MHz transmitter and 13-MHz receiver. Microbubbles in weak solutions were insonified with a 5-cycle pulse at a peak rarefactional pressure of 2.0+/-0.2 MPa. For each microbubble type, at least 100 received signals were identified as individual-microbubble responses. The average broadband noise from signals with postexcitation response was 4.2-7.2 dB higher than from signals without postexcitation. Pressure-time responses for each microbubble type were simulated using the model by Marmottant et al. [J. Acoust. Soc. Am. 118, 3499-3505 (2005)], with insonification conditions matching the experiment. Increased broadband noise predicted for microbubbles with postexcitation response was consistent with that observed experimentally (4.0-8.9 dB). The model predicted that postexcitation signals occur only when the radial oscillation exceeds both the shell break-up threshold and twice the initial radius (free bubble inertial cavitation threshold).

摘要

这项工作结合了建模和实验,以评估与微泡激发后检测到的宽带压力峰值(后激发信号)相关的封装微泡振荡。使用由共焦排列的 2.8MHz 发射器和 13MHz 接收器组成的被动空化探测器,从白蛋白壳和磷脂壳微泡中获取数据。在弱溶液中的微泡用 5 个周期的脉冲激励,峰值稀疏压力为 2.0+/-0.2 MPa。对于每种微泡类型,至少有 100 个接收信号被识别为单个微泡响应。具有后激发响应的信号的平均宽带噪声比没有后激发的信号高 4.2-7.2dB。使用 Marmottant 等人的模型模拟每种微泡类型的压力-时间响应[J. Acoust. Soc. Am. 118, 3499-3505 (2005)],激励条件与实验匹配。与实验观察到的情况一致,后激发响应的微泡预测的宽带噪声增加(4.0-8.9dB)。该模型预测,只有当径向振荡超过壳破裂阈值和初始半径的两倍(自由泡惯性空化阈值)时,才会发生后激发信号。