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Magn Reson Med. 2010 Jan;63(1):181-93. doi: 10.1002/mrm.22178.
3
Differential dose volume histograms of Gamma knife in the presence of inhomogeneities using MRI-polymer gel dosimetry and MC simulation.使用MRI-聚合物凝胶剂量测定法和蒙特卡罗模拟法得到的伽马刀在存在不均匀性情况下的剂量体积直方图差异。
Med Phys. 2009 Jul;36(7):3002-12. doi: 10.1118/1.3147256.
4
Calculating T2 in images from a phased array receiver.计算来自相控阵接收器的图像中的T2值。
Magn Reson Med. 2009 Apr;61(4):962-9. doi: 10.1002/mrm.21904.
5
Magnetization transfer proportion: a simplified measure of dose response for polymer gel dosimetry.磁化转移比例:聚合物凝胶剂量学剂量响应的一种简化测量方法。
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6
Carr-Purcell-Meiboom-Gill imaging of prostate cancer: quantitative T2 values for cancer discrimination.前列腺癌的卡尔-珀塞尔-梅博姆-吉尔成像:用于癌症鉴别的定量T2值
Magn Reson Imaging. 2009 May;27(4):497-502. doi: 10.1016/j.mri.2008.08.001. Epub 2008 Sep 26.
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基于 MRI 的聚合物凝胶剂量测定中 R2 估计的可变回波数方法。

A variable echo-number method for estimating R2 in MRI-based polymer gel dosimetry.

机构信息

Department of Therapeutic Radiology, University of Minnesota, Minneapolis, Minnesota 55455, USA.

出版信息

Med Phys. 2011 Feb;38(2):975-82. doi: 10.1118/1.3544659.

DOI:10.1118/1.3544659
PMID:21452734
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC3041809/
Abstract

PURPOSE

Spin-spin relaxation rate R2 is commonly used to quantify absorbed dose for magnetic resonance imaging (MRI)-based polymer gel dosimetry. R2 is estimated by applying a parameter fitting algorithm to a train of spin-echo signals. However, a careless application of a large number of echoes can result in anomalous R2 values because the echo signal intensity decreases to the background signal offset level for a long echo time. In this article, the authors proposed and evaluated a variable echo-number (VAREC) method to remedy the problem.

METHODS

The VAREC algorithm uses only echo signals, whose intensities are greater than a preset threshold. Here, the threshold is defined as the standard deviation of Gaussian noise times a multiplier alpha. The authors implemented three R2 estimation methods in an in-house program: The nonlinear least-squares algorithm (NLLS), the VAREC method, and the maximum likelihood estimator with the Rician signal intensity distribution (MLE_R). Those methods were used to estimate the R2 values of test phantoms with known R2 values and BANG3-type polymer gels, which were irradiated to 12 different doses ranging from 0 to 50 Gy. The R2 values were measured by using a 32-echo CPMG pulse sequence on 3 T MRI scanners. The R2 values of the VAREC method were compared with those of NLLS and MLE_R.

RESULTS

The R2 values of the NLLS method incorrectly decreased to the zero-dose level for doses greater than 10 Gy. The R2 values of the VAREC method with alpha=2 agreed with those of MLE_R within the measurement uncertainty. The uncertainties of the R2 values were the smallest for alpha=2 or 3 among various alpha values.

CONCLUSIONS

The VAREC algorithm is simple, fast, and robust for the R2 estimation. The authors recommend this method with alpha=2 or 3 for R2 estimation using multispin echo MRI protocols.

摘要

目的

自旋-自旋弛豫率 R2 常用于磁共振成像(MRI)基聚合物凝胶剂量测定中的吸收剂量定量。R2 通过对一组自旋回波信号应用参数拟合算法来估计。然而,大量回波的粗心应用可能会导致异常的 R2 值,因为回波信号强度对于长回波时间会降至背景信号偏移水平。在本文中,作者提出并评估了一种可变回波数(VAREC)方法来解决该问题。

方法

VAREC 算法仅使用强度大于预设阈值的回波信号。这里,阈值定义为高斯噪声的标准偏差乘以倍增器 alpha。作者在内部程序中实现了三种 R2 估计方法:非线性最小二乘算法(NLLS)、VAREC 方法和具有瑞利信号强度分布的最大似然估计器(MLE_R)。这些方法用于估计具有已知 R2 值的测试体模和 BANG3 型聚合物凝胶的 R2 值,这些体模被照射到 12 个从 0 到 50 Gy 的不同剂量。使用 3 T MRI 扫描仪上的 32 回波 CPMG 脉冲序列测量 R2 值。将 VARC 方法的 R2 值与 NLLS 和 MLE_R 的 R2 值进行比较。

结果

NLLS 方法的 R2 值对于大于 10 Gy 的剂量错误地降至零剂量水平。VAREC 方法的 R2 值与 MLE_R 在测量不确定度内一致。在各种 alpha 值中,alpha=2 或 3 的 R2 值的不确定度最小。

结论

VAREC 算法用于 R2 估计既简单又快速且稳健。作者推荐在使用多自旋回波 MRI 协议进行 R2 估计时使用此方法和 alpha=2 或 3。