使用单线圈的内部磁感应断层扫描

J. Feldkamp, S. Quirk
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引用次数: 5

摘要

大多数成像方式成像的是物体的内部,而所有的仪器,包括光源和接收器,都位于物体的外部。一个值得注意的例外是超声波(US),它可以小型化到足以在物体内定位US换能器并收集数据用于图像重建。另一种是井间地球物理成像。任何内部成像方式的目标都是提供更高保真度的图像,同时避免干扰结构。由于多线圈磁感应断层扫描(MIT)体积庞大,发射和接收线圈从未放置在小目标(如人体)内。在这里,我们展示了一种单线圈MIT的新实现,当线圈位于由盐掺杂琼脂糖组成的小型实验室制造的幻影内部时,它可以进行扫描。幻影的几何形状是环形的,由一个直径6.0厘米、深度5.5厘米的通道组成,周围是一个3.0厘米厚的圆柱形壁。一个嵌入的、位于中心位置的2.0 cm厚的琼脂糖凝胶环,加入足够的NaCl以提高其导电性,高于周围的琼脂糖。所得到的近乎轴对称的幻影由电导率范围为0.11至10.55 S/m的材料组成。扫描是机器人完成的,线圈存根安装在3轴控制器的定位头上,该控制器将平面圆形线圈定位到360或720个预设的内部位置。从收集到的数据中重建图像显示正确地揭示了近似轴对称夹杂物的位置、大小和电导率。
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INTERNAL MAGNETIC INDUCTION TOMOGRAPHY USING A SINGLE COIL
Most imaging modalities image an object’s interior while all instrumentation, including sources and receivers, is externally located. One notable exception is ultra-sound (US), which can be miniaturized sufficiently to locate a US transducer within an object and gather data for image reconstruction. Another is cross-borehole geophysical imaging. The goal of any internal imaging modality is to provide images of greater fidelity while avoiding interfering structures. Due to the bulkiness of multi-coil magnetic induction tomography (MIT), transmitting and receiving coils are never placed within small targets (e.g., a human body). Here, we demonstrate a novel implementation of single-coil MIT that performs a scan all while the coil is located within the interior of a small, labcreated phantom consisting of salt-doped agarose. Phantom geometry is annular, consisting of a 6.0 cm diameter channel of depth 5.5 cm surrounded by a 3.0 cm thick cylindrical wall. An embedded, centrally located agarose gel annulus, 2.0 cm thick, is doped with sufficient NaCl to elevate its conductivity above that of surrounding agarose. The resulting nearly axisymmetric phantoms consist of material having conductivity ranging from 0.11 to 10.55 S/m. A scan is accomplished robotically, with the coil stubmounted on the positioning head of a 3-axis controller that positions the planar circular loop coil into 360 or 720 preset internal positions. Image reconstruction from gathered data is shown to correctly reveal the location, size and conductivity of the approximately axisymmetric inclusion.
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