一种测量单微米大小物体的超声后向散射的新技术

O. Falou, Min Rui, Ahmed El-Kaffas, J. Kumaradas, Michael C. Kolios
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引用次数: 3

摘要

为了了解弱散射体(细胞)和强散射体(造影剂)的行为,需要测量来自单个微米大小物体的超声后向散射,用于从组织表征到分子成像的应用。然而,获得这样的回应仍然是一个挑战。例如,在测量细胞后向散射时,细胞悬浮液中气泡的存在可能导致对后向散射信号的不正确解释。此外,产生超声后向散射信号的单个物体的大小和形状是理论模型的关键输入参数,但很难在实验中测量。在这项工作中,开发了一种新技术,将Xenoworks显微注射系统(Sutter, Inc., Los Angeles, CA)与共同注册的Olympus IX71倒置显微镜(Olympus America, Inc., Center Valley, PA)和VEVO770超声成像设备(visualsonic, Inc., Toronto, ON)结合在一起,在光学显微镜引导下获得单个物体的超声后向散射响应。这项技术提供了关于物体大小和形状的准确信息。使用两个中心频率为25和55 MHz的换能器(总频谱为12-57 MHz)。将光学透镜和换能器的焦点对准,得到同一区域的光学和超声图像。将目标物附着在微移液管上(使用负压),然后从微移液管上释放(使用正压和/或轻敲微移液管),同时对其进行光学和超声成像。为了校准系统,使用微移管在−18.9 kPa的压力下从脱气水中的微球悬浮液中抓取20µm的聚苯乙烯微球。施加+35.0 kPa的压力释放微球。在释放过程中,获得了光学和超声原始射频线。然后用这些谱线得到单个微球的功率谱图,并与解析解进行比较。微球的后向散射响应与弹性球的Faran模型的后向散射响应非常吻合(误差为1%)。将该方法扩展到前列腺癌(PC-3)细胞,与Anderson流体球模型相比,结果吻合良好(误差为5%)。该技术能够提供来自单个物体的反向散射的精确测量,目前正用于推断来自不同大小的其他细胞系的反向散射响应,以及来自分离或附着在细胞上的超声造影剂的反向散射响应。讨论了该技术的优点及其未来的应用前景。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
A novel technique for measuring ultrasound backscatter from single micron-sized objects
The measurement of the ultrasound backscatter from individual micron-sized objects is required to gain an understanding of the behavior of both weak (cells) and strong (contrast agents) scatterers for applications ranging from tissue characterization to molecular imaging. However, obtaining such a response remains a challenge. For instance, the presence of air bubbles in a suspension of cells during measurements of cell backscatter may lead to the incorrect interpretation of the backscattered signals. In addition, the size and shape of the single object that produces an ultrasound backscatter signal are critical input parameters to theoretical models, yet hard to be measured experimentally. In this work, a novel technique combining a Xenoworks microinjection system (Sutter, Inc., Los Angeles, CA) with co-registered Olympus IX71 inverted microscope (Olympus America, Inc., Center Valley, PA) and a VEVO770 Ultrasound imaging device (VisualSonics, Inc., Toronto, ON) was developed in which the ultrasound backscatter response from a single object was obtained under optical microscope guidance. This technique provides accurate information about the size and shape of the object. Two transducers of central frequencies of 25 and 55 MHz were used (for a total spectrum of 12–57 MHz). The foci of the optical lens and the transducer were aligned to obtain optical and ultrasonic images of the same region. The object of interest was attached to the micropipette (using negative pressure) and then released from the micropipette (using positive pressure and/or tapping on the micropipette) while imaging it both optically and ultrasonically. In order to calibrate the system, a micropipette was used to grab a 20 µm polystyrene microsphere from a suspension of microspheres in degassed water by applying a pressure of −18.9 kPa. The microsphere was released by applying a pressure of +35.0 kPa. During the release, optical and ultrasonic raw RF lines were obtained. These lines were then used to obtain the power spectral plot of individual microspheres which were compared to analytical solutions. A very good agreement was found (error of 1%) between the measured backscatter response of microspheres and that of a Faran model of an elastic sphere. Extension of this method to prostate carcinoma (PC-3) cells showed a good agreement (error of 5%) when compared to the Anderson fluid sphere model. This technique is capable of providing accurate measurements of the backscatter from individual objects and is currently being used to deduce the backscatter response from other cell lines of different sizes and from ultrasound contrast agents either in isolation or when attached to a cell. The advantages of the technique along with its future applications are discussed.
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