Pouliopoulos Antonios N, Choi James J
Noninvasive Surgery and Biopsy laboratory, Bioengineering Department, Imperial College London, London SW7 2AZ, UK.
Phys Med Biol. 2016 Aug 21;61(16):6154-71. doi: 10.1088/0031-9155/61/16/6154. Epub 2016 Jul 29.
The introduction of microbubbles in focused ultrasound therapies has enabled a diverse range of non-invasive technologies: sonoporation to deliver drugs into cells, sonothrombolysis to dissolve blood clots, and blood-brain barrier opening to deliver drugs into the brain. Current methods for passively monitoring the microbubble dynamics responsible for these therapeutic effects can identify the cavitation position by passive acoustic mapping and cavitation mode by spectral analysis. Here, we introduce a new feature that can be monitored: microbubble effective velocity. Previous studies have shown that echoes from short imaging pulses had a Doppler shift that was produced by the movement of microbubbles. Therapeutic pulses are longer (>1 000 cycles) and thus produce a larger alteration of microbubble distribution due to primary and secondary acoustic radiation force effects which cannot be monitored using pulse-echo techniques. In our experiments, we captured and analyzed the Doppler shift during long therapeutic pulses using a passive cavitation detector. A population of microbubbles (5 × 10(4)-5 × 10(7) microbubbles ml(-1)) was embedded in a vessel (inner diameter: 4 mm) and sonicated using a 0.5 MHz focused ultrasound transducer (peak-rarefactional pressure: 75-366 kPa, pulse length: 50 000 cycles or 100 ms) within a water tank. Microbubble acoustic emissions were captured with a coaxially aligned 7.5 MHz passive cavitation detector and spectrally analyzed to measure the Doppler shift for multiple harmonics above the 10th harmonic (i.e. superharmonics). A Doppler shift was observed on the order of tens of kHz with respect to the primary superharmonic peak and is due to the axial movement of the microbubbles. The position, amplitude and width of the Doppler peaks depended on the acoustic pressure and the microbubble concentration. Higher pressures increased the effective velocity of the microbubbles up to 3 m s(-1), prior to the onset of broadband emissions, which is an indicator for high magnitude inertial cavitation. Although the microbubble redistribution was shown to persist for the entire sonication period in dense populations, it was constrained to the first few milliseconds in lower concentrations. In conclusion, superharmonic microbubble Doppler effects can provide a quantitative measure of effective velocities of a sonicated microbubble population and could be used for monitoring ultrasound therapy in real-time.
在聚焦超声治疗中引入微泡,催生了一系列非侵入性技术:用于将药物输送到细胞内的声孔效应、用于溶解血栓的超声溶栓以及用于将药物输送到脑内的血脑屏障开放。目前用于被动监测产生这些治疗效果的微泡动力学的方法,可以通过被动声学成像确定空化位置,并通过频谱分析确定空化模式。在此,我们介绍一种可以监测的新特性:微泡有效速度。此前的研究表明,短成像脉冲产生的回波存在由微泡运动引起的多普勒频移。治疗脉冲更长(>1000个周期),因此由于一次和二次声辐射力效应,会使微泡分布产生更大变化,而这无法用脉冲回波技术进行监测。在我们的实验中,我们使用被动空化探测器在长治疗脉冲期间捕获并分析了多普勒频移。将一群微泡(5×10⁴ - 5×10⁷个微泡/毫升)注入内径为4毫米的血管中,并在水箱内使用0.5兆赫聚焦超声换能器(峰值稀疏压力:75 - 366千帕,脉冲长度:50000个周期或100毫秒)进行超声处理。用同轴对齐的7.5兆赫被动空化探测器捕获微泡声发射,并进行频谱分析,以测量高于第10谐波(即超谐波)的多个谐波的多普勒频移。相对于初级超谐波峰值,观察到的多普勒频移在几十千赫量级,这是由微泡的轴向运动引起的。多普勒峰值的位置、幅度和宽度取决于声压和微泡浓度。在宽带发射开始之前,较高的压力会使微泡的有效速度增加到3米/秒,这是高强度惯性空化的一个指标。尽管在密集群体中,微泡重新分布在整个超声处理期间都持续存在,但在较低浓度下,它被限制在前几毫秒内。总之,超谐波微泡多普勒效应可以提供超声处理微泡群体有效速度的定量测量,可用于实时监测超声治疗。