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磁化率作为一种与B0场强无关的肝脏铁过载MRI生物标志物。

Magnetic susceptibility as a B0 field strength independent MRI biomarker of liver iron overload.

作者信息

Hernando Diego, Cook Rachel J, Diamond Carol, Reeder Scott B

机构信息

Department of Radiology, University of Wisconsin, Madison, Wisconsin, USA.

出版信息

Magn Reson Med. 2013 Sep;70(3):648-56. doi: 10.1002/mrm.24848. Epub 2013 Jun 25.

Abstract

PURPOSE

MR-based quantification of liver magnetic susceptibility may enable field strength-independent measurement of liver iron concentration (LIC). However, susceptibility quantification is challenging, due to nonlocal effects of susceptibility on the B0 field. The purpose of this work is to demonstrate feasibility of susceptibility-based LIC quantification using a fat-referenced approach.

METHODS

Phantoms consisting of vials with increasing iron concentrations immersed between oil/water layers, and 27 subjects (9 controls/18 subjects with liver iron overload) were scanned. Ferriscan (1.5 T) provided R2-based reference LIC. Multiecho three-dimensional-SPGR (1.5 T/3 T) enabled fat-water, B0- and R2*-mapping. Phantom iron concentration (mg Fe L(-1)) was estimated from B0 differences (ΔB0) between vials and neighboring oil. Liver susceptibility and LIC (mg Fe g(-1) dry tissue) was estimated from ΔB0 between the lateral right lobe of the liver and adjacent subcutaneous adipose tissue.

RESULTS

Estimated phantom iron concentrations had good correlation with true iron concentrations (1.5 T:slope = 0.86, intercept = 0.72, r(2) = 0.98; 3 T:slope = 0.85, intercept = 1.73, r(2) = 0.98). In liver, ΔB0 correlated strongly with R2* (1.5 T:r(2) = 0.86; 3 T:r(2) = 0.93) and B0-LIC had good agreement with Ferriscan-LIC (slopes/intercepts nearly 1.0/0.0, 1.5 T:r(2) = 0.67, slope = 0.93 ± 0.13, P ≈ 0.50, intercept = 1.93 ± 0.78, P ≈ 0.02; 3 T:r(2) = 0.84, slope = 1.01 ± 0.09, P ≈ 0.90, intercept = 0.23 ± 0.52, P ≈ 0.68).

DISCUSSION

Fat-referenced, susceptibility-based LIC estimation is feasible at both field strengths. This approach may enable improved susceptibility mapping in the abdomen.

摘要

目的

基于磁共振成像的肝脏磁化率定量分析可实现与场强无关的肝脏铁浓度(LIC)测量。然而,由于磁化率对B0场的非局部效应,磁化率定量分析具有挑战性。本研究的目的是证明使用脂肪参考方法进行基于磁化率的LIC定量分析的可行性。

方法

扫描由浸于油/水层之间、铁浓度递增的小瓶组成的体模,以及27名受试者(9名对照/18名肝脏铁过载受试者)。Ferriscan(1.5T)提供基于R2的参考LIC。多回波三维扰相梯度回波序列(1.5T/3T)可实现脂肪-水、B0和R2*成像。根据小瓶与相邻油之间的B0差异(ΔB0)估算体模铁浓度(mg Fe L(-1))。根据肝脏右叶外侧与相邻皮下脂肪组织之间的ΔB0估算肝脏磁化率和LIC(mg Fe g(-1)干组织)。

结果

估算的体模铁浓度与真实铁浓度具有良好的相关性(1.5T:斜率 = 0.86,截距 = 0.72,r(2) = 0.98;3T:斜率 = 0.85,截距 = 1.73,r(2) = 0.98)。在肝脏中,ΔB0与R2*密切相关(1.5T:r(2) = 0.86;3T:r(2) = 0.93),且B0-LIC与Ferriscan-LIC具有良好的一致性(斜率/截距接近1.0/0.0,1.5T:r(2) = 0.67,斜率 = 0.93 ± 0.13,P ≈ 0.50,截距 = 1.93 ± 0.78,P ≈ 0.02;3T:r(2) = 0.84,斜率 = 1.01 ± 0.09,P ≈ 0.90,截距 = 0.23 ± 0.52,P ≈ 0.68)。

讨论

基于脂肪参考的、基于磁化率的LIC估测在两种场强下均可行。该方法可能有助于改善腹部的磁化率成像。

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