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

机译:PA成像通过窄光束扫描和单次宽梁激励的比较

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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 firing 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 (-j 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 x 10 mm in cross section and acted as the broad beam; the other was 5 mm x 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:专为深光声(PA)成像设计的电流系统通常使用低重复率,高功率脉冲激光器提供NS级脉冲照明大组织体积。记录在每个激光射击上的声学信号可用于重建该区域内的热释放源的完整2-D(3-D)图像。使用宽梁激励,成像系统的最大帧速率受激光脉冲重复率的限制。基于沿着感兴趣区域的组织表面通过低能量(-J 1 MJ)高重复率(-1mm)的低能量(-J 1 MJ)高重复率(最多几kHz)窄激光束(-1mm)来提出替代的照明方法。从在每个激光束位置重建的单独PA图像的总和的总和产生最终PA图像。该概念可以利用高重复率光纤激光器,以创建具有比当前系统更高的帧速率的PA图像,从而实现具有超声成像的光声学的真正实时集成。作为概念的初始证明,我们将传统的宽波束照明与简单模型系统中的扫描光束方法进行比较。直径为1.6mm和0.8mm的两个透明的Teflon管填充吸收系数为5cm〜(-1)的油墨。将这些管埋在用作光学散射介质的鸡胸组织内。它们分隔3 mm或10 mm,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。激励源是由Q开关的ND:YAG激光带有倍增器的传统的OPO。使用来自扫描的PVDF换能器的信号重建光声图像,该信号用作声学阵列。比较两种不同的照明方案:横截面中的一个是15mm×10mm,并用作宽梁;另一个是5mm×2mm的横截面(比宽梁壳小15倍),并在相当于宽波束照明的区域上扫描。在窄光束扫描期间获得的多个图像一起加入以形成等于单射宽光束的PA图像。 Phantom研究的结果表明,通过窄光束扫描激励形成的PA图像可以等于信号到噪声比和空间分辨率的一个镜头宽波束照明。未来的研究将专注于高重复速率激光源和适合实时,集成深光声/超声成像的扫描格式。

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