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Photoacoustic Imaging Paradigm Shift: Towards Using Vendor-Independent Ultrasound Scanners

机译:光声成像范式班次:朝着使用不合贩子的超声扫描仪

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Photoacoustic (PA) imaging requires channel data acquisition synchronized with a laser firing system. Unfortunately, the access to these channel data is only available on specialized research systems, and most clinical ultrasound scanners do not offer an interface to obtain this data. To broaden the impact of clinical PA imaging, we propose a vendor-independent PA imaging system utilizing ultrasound post-beamformed radio frequency (RF) data, which is readily accessible in some clinical scanners. In this paper, two PA beamforming algorithms that use the post-beamformed RF data as the input are introduced: inverse beamforming, and synthetic aperture (SA) based re-beamforming. Inverse beamforming recovers the channel data by taking into account the ultrasound beamforming delay function. The recovered channel data can then be used to reconstruct a PA image. SA based re-beamforming algorithm regards the defocused RF data as a set of pre-beamformed RF data received by virtual elements; an adaptive synthetic aperture beamforming algorithm is applied to refocus it. We demonstrated the concepts in simulation, and experimentally validated their applicability on a clinical ultrasound scanner using a pseudo-PA point source and in vivo data. Results indicate the full width at the half maximum (FWHM) of the point target using the proposed inverse beamforming and SA re-beamforming were 1.33 mm, and 1.08 mm, respectively. This is comparable to conventional delay-and-sum PA beamforming, for which the measured FWHM was 1.49 mm.
机译:光声(PA)成像需要与激光发射系统同步的信道数据采集。不幸的是,对这些频道数据的访问仅适用于专业的研究系统,而大多数临床超声扫描仪不提供界面以获得此数据。为了拓宽临床PA成像的影响,我们提出了一种利用超声波波束形成射频(RF)数据的供应商独立的PA成像系统,该系统在某些临床扫描仪中易于访问。在本文中,引入了两个PA波束成形算法,其使用后波束形成的RF数据作为输入:逆波束成形和基于合成孔径(SA)的重新波束成形。逆波束成形通过考虑超声波形成延迟功能来恢复信道数据。然后可以使用恢复的信道数据来重建PA图像。基于SA的重新波束成形算法将Defocused RF数据视为虚拟元素接收的一组预先波束形成的RF数据;自适应合成孔径波束成形算法应用于重新焦点。我们展示了仿真中的概念,并通过伪PA点源和体内数据进行了实验验证了他们在临床超声扫描仪上的适用性。结果使用所提出的逆波束形成和SA重新波束形成的点目标的半峰值(FWHM)的全宽分别为1.33mm,1.08mm。这与传统的延迟和和PA波束形成相当,测量的FWHM为1.49mm。

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