Natural D-glucose can serve as a biodegradable contrast agent for the detection of tumors by means of Chemical Exchange Saturation Transfer (CEST) or Chemical Exchange sensitive Spin-Lock (CESL) Dynamic Glucose Enhanced (DGE) MRI. For application of CESL-based DGE-MRI at a 7T whole-body scanner, we implemented an adiabatic CESL sequence and essentially increased the temporal resolution employing a T1ρ-weighted acquisition scheme. Further, we introduced a simple, robust and quantitative DGE contrast. First application of T1ρ-weighted DGE-MRI in a glioblastoma patient provided a substantial contrast between tumor and healthy brain tissue and showed the dynamic glucose enhancement after a glucose bolus injection.
For a two-pool system, e.g. protons of water and glucose, the on-resonant relaxation rate in the rotating frame (R1ρ) is given by R1ρ = R2 + Rex. The exchange dependent relaxation rate (Rex) is a linear function of the relative glucose concentration (cGlc) and is given by6
$$ R_{ex} = c_{Glc}\cdot\frac{k\cdot\delta^2}{\delta^2+4\pi^2\omega_1^2+k^2} $$
For T1ρ-weighted MRI we could show that the difference in signal intensities between a voxel-of-interest and a reference voxel with different exchange-dependent relaxation can be approximated by5
$$ \Delta S =S_{ref}-S \approx \Delta R_{ex} \cdot TSL \cdot e^{-R_{1\rho} \cdot TSL} $$
assuming that ΔRex∙TSL << 1, where TSL is the spin-lock time. This formula also holds for the same voxel but different time points, e.g. in T1ρ-weighted DGE-MRI before and after administration of glucose. Dividing ΔS by the reference signal Sref yields the T1ρ-weighted dynamic glucose enhancement (DGEρ), which is independent of relaxation parameters of tissue and solely depends on the glucose concentration change for a given TSL:
$$ DGE_{\rho}=\frac{S_{ref}-S}{S_{ref}} \approx \Delta c_{glc} \cdot TSL $$
To confirm that DGEρ does not depend on the relaxation parameters of tissue we
performed measurements on aqueous model solutions with different
glucose concentrations and different relaxation rates. Despite
the different relaxation curves (Fig. 1a), DGEρ as a
function of ΔcGlc agrees well for both phantoms and shows the
linear dependence expected from theory (Fig 1b). Thus, DGEρ
reflects a quantitative contrast that solely depends on changes of the glucose concentration. This is similar to ΔR1ρ employing R1ρ mapping, which, however, suffers from a tenfold longer acquisition time if applied to studies in humans5.
Figure 2 shows the results of a first examination of a brain tumor patient with T1ρ-weighted DGE-MRI. The DGEρ image obtained about 8 minutes after glucose injection (Fig. 2c) clearly highlights the tumor region consistent with the T2-weighted (Fig. 2a) and gadolinium enhanced T1-weighted images (Fig. 2b). An increased DGEρ contrast was also observed in the ventricular area and in another region at the bottom of the tumor area. T1ρ-weighted DGE-MRI allowed investigating the glucose contrast with a temporal resolution of less than seven seconds in three regions of interest: 1) the glucose enhancing region, 2) the gadolinium enhancing region and 3) normal appearing white matter (NAWM). The ROI-specific curves are displayed in figure 2d. After the start of the injection (t = 0 min) all curves increase. However, NAWM shows only a minor increase compared with the tumor ROIs. The highest DGEρ values were observed in the tumor region about 10 min after start of the injection; the subsequent signal drop most likely results from patient motion.
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