Assessing the limits of MPI tracer performance

R. M. Ferguson, A. Khandhar, H. Arami, S. Conolly, K. Krishnan
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引用次数: 1

Abstract

Simulations of m'(H) (Fig 1B), which matched MPS (Fig 1C, D) and PSFs (Fig 1A), can be used to predict tracer behavior during imaging. Under applied field conditions commonly used in MPI (25 kHz, 20 mT/μ0), our model predicts that hysteresis will appear in m(H) loops for particles larger than 20 nm diameter, when Keff is 6000 [J m-3], which is the average Keff measured for our MPI tracer. Due to thermal fluctations, the model predicts a maximum coercive field that is less than predicted by the original Stoner-Wohlfarth model, which is given by 2Keff/Ms, where MS, is the saturation magnetization. For a fixed value of Keff, the model predicts that coercive field increases with median particle size, however the FWHM of m'(H) remains relatively unchanged as the loop opens up with increasing particle size. In simulations, the FWHM of m'(H) decreased with Keff. The minimum FWHM predicted by the model when Keff is 6000 was 5 mT; this was consistent with the measured FWHM (5.5 mT) for 25 nm tracers.
评估MPI示踪剂性能的极限
模拟m′(H)(图1B)与MPS(图1C, D)和psf(图1A)相匹配,可用于预测成像过程中的示踪剂行为。在MPI常用的应用场强条件下(25 kHz, 20 mT/μ0),我们的模型预测,当Keff为6000 [J m-3]时,对于直径大于20 nm的粒子,我们的MPI示踪剂测量到的平均Keff为6000 [J m-3], m(H)环将出现迟滞。由于热波动,该模型预测的最大矫顽力场小于原Stoner-Wohlfarth模型预测的最大矫顽力场,由2Keff/Ms给出,其中Ms为饱和磁化强度。在一定的Keff值下,模型预测矫顽力场随着中位粒径的增大而增大,而m′(H)的FWHM随着环开度的增大保持相对不变。在模拟中,m′(H)的FWHM随Keff的增大而减小。当Keff为6000时,模型预测的最小FWHM为5 mT;这与25 nm示踪剂的FWHM (5.5 mT)一致。
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