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Comparison of PA imaging by narrow beam scanning and one-shot broad beam excitation

机译:窄束扫描和单次宽束激发对PA成像的比较

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Current systems designed for deep photoacoustic (PA) imaging typically use a low repetition rate, high power pulsed laser to provide a ns-scale pulse illuminating a large tissue volume. Acoustic signals recorded on each laser tiring can be used to reconstruct a complete 2-D (3-D) image of sources of heat release within that region. Using broad-beam excitation, the maximum frame rate of the imaging system is restricted by the pulse repetition rate of the laser. An alternate illumination approach is proposed based on fast scanning by a low energy (~ 1 mJ) high repetition rate (up to a few kHz) narrow laser beam (~1 mm) along the tissue surface over a region of interest. A final PA image is produced from the summation of individual PA images reconstructed at each laser beam position. This concept can take advantage of high repetition rate fiber lasers to create PA images with much higher frame rates than current systems, enabling true real-time integration of photoacoustics with ultrasound imaging. As an initial proof of concept, we compare conventional broad beam illumination to a scanned beam approach in a simple model system. Two transparent teflon tubes with diameters of 1.6 mm and 0.8 mm were filled with ink having an absorption coefficient of 5 cm~(-1). These tubes were buried inside chicken breast tissue acting as an optical scattering medium. They were separated by 3 mm or 10 mm to test spatial and contrast resolution for the two scan formats. The excitation wavelength was 700 nm. The excitation source is a traditional OPO pumped by a Q-switched Nd:YAG laser with doubler. Photoacoustic images were reconstructed using signals from a small, scanned PVDF transducer acting as an acoustic array. Two different illumination schemes were compared: one was 15 mm × 10 mm in cross section and acted as the broad beam; the other was 5 mm × 2 mm in cross section (15 times smaller than the broad beam case) and was scanned over an area equivalent to broad beam illumination. Multiple images obtained during narrow beam scanning were added together to form one PA image equivalent to the single-shot broad beam one. Results of the phantom study indicate that PA images formed by narrow beam scanning excitation can be equivalent to one shot broad beam illumination in signal to noise ratio and spatial resolution. Future studies will focus on high repetition-rate laser sources and scan formats appropriate for real-time, integrated deep photoacoustic/ultrasonic imaging.
机译:设计用于深光声(PA)成像的当前系统通常使用低重复频率,高功率脉冲激光来提供ns尺度的脉冲,以照亮较大的组织体积。记录在每个激光疲劳上的声信号可用于重建该区域内放热源的完整2-D(3-D)图像。使用宽光束激发,成像系统的最大帧速率受到激光脉冲重复率的限制。提出了一种替代照明方法,该方法基于在感兴趣区域上沿着组织表面的低能量(〜1 mJ)高重复率(高达几kHz)窄激光束(〜1 mm)进行快速扫描。根据在每个激光束位置重建的单个PA图像的总和生成最终的PA图像。该概念可以利用高重复频率的光纤激光器来创建具有比当前系统高得多的帧频的PA图像,从而实现光声与超声成像的实时集成。作为概念的初步证明,我们将传统的宽光束照明与简单模型系统中的扫描光束方法进行了比较。在两个直径为1.6 mm和0.8 mm的透明聚四氟乙烯管中填充吸收系数为5 cm〜(-1)的墨水。这些管被埋在充当光学散射介质的鸡胸组织内部。将它们分开3毫米或10毫米,以测试两种扫描格式的空间和对比度分辨率。激发波长为700nm。激发源是传统的OPO,由带有倍频器的Q开关Nd:YAG激光器泵浦。使用来自作为声阵列的小型扫描PVDF换能器的信号重建光声图像。比较了两种不同的照明方案:一种是横截面为15 mm×10 mm,并用作宽光束。另一个的横截面为5 mm×2 mm(比宽光束情况小15倍),并在相当于宽光束照明的区域上进行扫描。在窄光束扫描过程中获得的多幅图像被加在一起,以形成一张与单幅宽光束相同的PA图像。幻像研究的结果表明,由窄光束扫描激发形成的PA图像在信噪比和空间分辨率方面可以等同于一次发射的宽光束照明。未来的研究将集中于高重复频率的激光源和适合于实时,集成的深光声/超声成像的扫描格式。

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