Nonheme iron is an important element supporting the structure and functioning of biological tissues. Misbalance in nonheme iron can lead to different neurological disorders. Several MRI approaches have been developed for iron quantification relying either on the relaxation or susceptibility features of MRI signal. Specific quantification of the nonheme iron can, however, be tempered by the heme iron in the deoxygenated blood. The goal of this presentation is to introduce theoretical background and experimental method allowing disentangling contributions of heme and nonheme irons simultaneously with evaluation of tissue neuronal density in the basal ganglia.
METHODS
In this study we use qGRE technique that is based on 3D GRE MRI sequence with multiple gradient echoes, theoretical model7,8 of BOLD effect, and algorithms that we have developed for correcting adverse effects of background field gradients9 and physiological fluctuations10. qGRE data were acquired on Siemens 3T scanner Trio and 32 channel RF coil with FOV 256x192x144 mm, repetition time TR=50 ms, flip angle 35°, 10 gradient echoes with first echo time TE1 = 4 ms, echo spacing ∆TE = 4ms, voxel size (1x1x2 mm3). Phase stabilization echo was collected for each line in k-space to correct for image artefacts due to the physiological fluctuations. Raw k-space data are analyzed in MATLAB. The multi-channel data are combined using the previously published algorithm11. 3D spatial Hanning filter is applied to reduce Gibbs ringing artefacts and increase signal-to-noise ratio. Data are analyzed using theoretical model12 allowing disentanglement of tissue-cellular-specific (R2t*) and BOLD-related contributions to the total GRE MRI signal decay:
$$S(TE)=S_0\cdot exp(-R2t^*\cdot TE-i\omega\cdot TE)\cdot F_{BOLD}(\delta\omega,dCBV,TE)\cdot F_{macro}(TE)$$
where S(0) is the GRE signal intensity amplitude, TE is the gradient echo time, the function Fmacro(TE) accounts for the adverse effects of macroscopic magnetic field inhomogeneities9, and function FBOLD(TE) accounts for the BOLD contributions, δω is characteristic frequency and dCBV is deoxygenated blood volume7,12. Detailed description of the qGRE data analysis is available in12. Parameters δω and dCBV allow calculating a part of magnetic susceptibility related to the presence of heme iron in deoxyhemoglobin:
$$\chi_{deoxyhemoglobin}=\frac{3\cdot dCBV\cdot\delta\omega}{2\pi f_0}$$
where f0 is the scanner resonance frequency. $$$\chi_{deoxyhemoglobin}$$$ can be converted into concentration of deoxyhemoglobin $$$C_{deoxyhemoglobin}[mol/mL]=1.62\cdot \chi_{deoxyhemoglobin}$$$ 12. qGRE signal frequency ω is used to generate QSM maps using the algorithm developed in reference4. The nonheme iron-related magnetic susceptibility can then be calculated as follows:
$$\chi_{nonheme iron}=QSM-\chi_{deoxyhemoglobin}$$
Data were obtained from 22 healthy control subjects (ages 26-63 years) with local IRB approval.
RESULTS AND DISCUSSION
In13, using a multi-modality approach that included qGRE and Allen Human Brain Atlas gene expression data, we demonstrated that the R2t* metric of qGRE signal provides a unique genetic perspective of brain cortical structure and allows in vivo quantitative evaluation of brain neuronal, synaptic and glial cells densities. However, in regions of the brain with high iron accumulation R2t* is also affected by the relaxation processes induced by the water-iron interaction. To account for this phenomenon, three ROIs (caudate, putamen and pallidum) were segmented in each of 22 participants, combined in a single dataset and analyzed using the above-described methods. The regression analysis of R2t* vs. $$$\chi_{nonheme iron}$$$ and age resulted in:
$$R2t^*=14.3+123.2\chi_{nonheme iron}$$
with R2=0.83 and no significant age dependence (P=0.68). The neuronal index (NI) (parameter proportional to volume fraction of neurons) can be calculated from R2t*13 and is NI=0.42. This result suggests that the concentration of neurons in the basal ganglia remains constant across ages. As presented in Figs.2-4, the magnetic susceptibility of heme iron in deoxyhemoglobin only slightly increases with age, while concentration of nonheme iron increases with age significantly, especially in the pallidum. Since magnetic behavior of nonheme iron is not purely paramagnetic14 it would require additional assumptions to convert $$$\chi_{nonheme iron}$$$ into iron molar concentration. One of the important conclusions from our result is a significant contribution of heme iron to QSM measurements.
CONCLUSION
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