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Diffusion effects on NMR transverse relaxation around randomly distributed capillaries
Lukas Reinhold Buschle1,2, Christian H Ziener1, Martin Rückl3, Ke Zhang1,2, Volker J Sturm1,2, Gergely M Solecki4, Frank Winkler4, Martin Bendszus2, Sabine Heiland2, Heinz-Peter Schlemmer1, and Felix T Kurz1,2

1E010 Radiology, German Cancer Research Center, Heidelberg, Germany, 2Neuroradiology, University Hospital Heidelberg, Heidelberg, Germany, 3Department of Physics, Humboldt University Berlin, Berlin, Germany, 4Neurooncology, German Cancer Research Center, Heidelberg, Germany

Synopsis

The gradient echo and spin echo signal in brain tissue depend both on diffusion and susceptibility effects around and from capillaries, i.e. on structural and functional information that arise from the microvascular networks. In this work, the dependence of the relaxation rates R2 and R2* on capillary radius are considered for a random arrangement of capillaries in the strong collision approximation, and a closed-form solution is derived. Radius maps are then constructed for glioblastoma mice (N=8) to reveal an increased vessel radius in tumorous tissue as compared to non-affected brain tissue.

Target audience

The present work targets MR physicists and physicians with an interest in quantitative neuroimaging.

Purpose

A missing response to antiangiogenic therapy is considered a terminal situation for glioblastoma patients. However, monitoring treatment response is difficult since microvascular changes happen well below the conventional resolution of MR scanners in clinical routine. In this work, we consider both susceptibility and diffusion effects around random arrangements of capillaries in the strong collision approximation to derive a closed-form solution that connects relaxation rate and mean capillary radius.

Methods

We base our analysis on the well-known model of Yablonskiy and Haacke [1] that describes capillaries as infinitely long, parallel cylinders with a random arrangement and a constant diameter, which is applicable for low capillary volume fractions. Due to the BOLD-effect, each capillary then causes a change of the local Larmor frequency $$$\omega(\mathbf{r})$$$ in form of a dipole field: $$$\omega(\mathbf{r})=\delta\omega R^2\sum_i \frac{\cos(2\phi_i)}{r_i^2}\,,$$$ where $$$\delta\omega=2\pi\gamma B_0\Delta\chi\sin^2(\theta)$$$ is the strength of the dipole field, $$$R$$$ the capillary radius and $$$(r_i,\phi_i)$$$ are the coordinates of the i-th capillary. Diffusion effects can then be included in the weak-field [2] and the strong-collision approximation [3] to obtain closed-form solution of the spin echo and gradient echo signal in dependence on the capillary radius.

Random walk simulations to obtain gradient echo and spin echo signal were performed with a custom-made C++ code that uses 25000 random walk trajectories for each data point, see Fig. 1.

Animal experiments were performed to obtain capillary radius maps in tumorous and non-tumorous tissue of glioblastoma mice. In total eight 8-10 week old male NMRI nude mice (Charles River Laboratories, Sulzfeld, Germany) were used. A volume of 1 μL (50 000 tumor cells of glioblastoma cell line U87MG ATCC) were stereotactly implanted into the brain cortex in a depth of 500 μm [4]. MR images were obtained on day 28 after tumor implantation at a 9.4 T horizontal bore MR scanner (BioSpec 94/20 USR, Bruker BioSpin GmbH) with a four channel phased array surface coil. Quantitative $$$T_2$$$-maps were measured with a RARE sequence and $$$T_2^*$$$-maps were obtained from a multiecho gradientecho sequence. Dynamic susceptibility contrast (DSC) measurements were performed to acquire cerebral blood volume fractions. Sequence details are provided in Tab.1.

The relaxation rate $$$R_2^*$$$ and cerebral blood volume $$$\eta$$$ were used to calculate the dipole field strength $$$\delta\omega$$$. Spin echo signal, cerebral blood volume and dipole field strength are then used to obtain the capillary radius using the slow-diffusion approximation and assuming a diffusion coefficient of $$$D=1\mu\text{m}^2/ms$$$.

Results

Gradient echo signals are shown in Fig.2: for large capillaries, the relaxation rate $$$R_2^{*}$$$ coincides with the results of Yablonskiy and Haacke. For decreasing radii, diffusion effects lead to an averaging of the experienced magnetic field inhomogeneities and the relaxation rate $$$R_2^{*}$$$ decreases. Random walk simulations agree very well with the weak-field approximation for small capillary radii. However, the strong collision approximation shows a better agreement over the full range of the considered radii.

Since the spin echo signal is inverted at $$$t=TE/2$$$, the spin echo relaxation rate vanishes for large capillary radii (see Fig.2). With decreasing radii, diffusion effects lead to a displacement of spin-bearing particles and the inversion cannot recover the original magnetization (see Fig.1). For very small capillary radii, the spin echo relaxation rate agrees very well with the weak-field model, for large capillary radii, it agrees with the slow diffusion model [6].

The calculated mean capillary radius in mouse brains shows a significantly increased capillary radius inside the tumor tissue compared to healthy tissue (see Fig. 3 and Fig. 4).

Discussion

Our simulations suggest that, for radii $$$R > 1\mu\text{m}$$$, relaxation rates $$$R_2$$$ and $$$R_2^{*}$$$ are well-described by the slow diffusion approximation and static dephasing limit, respectively. The mean capillary radii in tumor tissue were about 30% larger than in non-affected tissue, in agreement with [7].

It should be noted that we require the dipole field strength to remain constant during measurements which is a reasonable assumption under stable vital conditions. The dipole field strength then provides information on the oxygen extraction fraction, see also [1], however, the weighting between arterial and venous fractions cannot be differentiated. Finally, our method is a promising tool to quantitatively characterize the microvasculator of tumorous tissue that can very easily be embedded into clinical routine.

Acknowledgements

This work was supported by grants from the Deutsche Forschungsgemeinschaft (Contract Grant number: DFG ZI 1295/2-1 and DFG KU 3555/1-1). F. T. Kurz was supported by a postdoctoral fellowship from the medical faculty of Heidelberg University and the Hoffmann-Klaus foundation of Heidelberg University.

References

[1] D. A. Yablonskiy and E. M. Haacke. Theory of NMR signal behavior in magnetically inhomogeneous tissues: the static dephasing regime. Magn Reson Med, 32:749–763, 1994.

[2] J. H. Jensen and R. Chandra. NMR relaxation in tissues with weak magnetic inhomogeneities. Magn Reson Med, 44:144–156, 2000.

[3] W. R. Bauer, W. Nadler, M. Bock, L. R. Schad, C. Wacker, A. Hartlep, G. Ertl. Theory of the BOLD effect in the capillary region: an analytical approach for the determination of T2 in the capillary network of myocardium. Magn Reson Med, 41:51–62, 1999.

[4] L. von Baumgarten, D. Brucker, A. Tirniceru, Y. Kienast, S. Grau, S. Burgold, J. Herms, F. Winkler. Bevacizumab has differential and dose-dependent effects on glioma blood vessels and tumor cells. Clin Cancer Res, 17:6192–6205, 2011.

[5] B. P. Chugh, J. P. Lerch, X. Y. Lisa, M. Pienkowski, R. V. Harrison, R. M. Henkelman, J. G.Sled. Measurement of cerebral blood volume in mouse brain regions using micro-computed tomography. Neuroimage, 47:1312–1318, 2009.

[6] V. G. Kiselev, R. Strecker, S. Ziyeh, O. Speck, J. Hennig. Vessel size imaging in humans. Magn Reson Med, 53:553-563, 2005.

[7] M. O. Breckwoldt et al. Correlated magnetic resonance imaging and ultramicroscopy (MR-UM) is a tool kit to assess the dynamics of glioma angiogenesis. eLife, 5:e11712, 2016.

Figures

Fig.1: Numerical random walk simulations of the spin echo signal for $$$TE=40ms$$$. For small capillary radii (a), diffusion effects prevent a rephasing of the magnetization. With increasing capillary radii ((b) and (c)), the spin echo becomes stronger and converges towards $$$t \to TE$$$.

Tab.1: TE and TR for the utilized sequences. $$$T_2$$$-, $$$T_2^*$$$-, DSC- maps as well as $$$T_1$$$-weighted images were obtained. DSC measurements were obtained before, during and after the bolus injection of the amount 0.1 mmol/kg of Gd-DTPA contrast agent with 4mL/s. $$$T_1$$$-weighted images were obtained after the injection.

Fig.2: Relaxation rate $$$R_2$$$ and $$$R_2^*$$$ in dependence on the capillary radius. For small radii, the relaxation process is well described by the weak-field approximation. The gradient echo simulation points over the full range of radii are well described by our closed-form solution of dephasing in the strong collision approximation.

Fig.3: (a) $$$T1$$$-weighted post-contrast image, (b) $$$CBV$$$-map, (c) $$$R_2$$$- and (d) $$$R_2^*$$$-map. (e) Dipole field strength $$$\delta\omega$$$-map calculated from the gradient echo signal, (f) mean capillary radius $$$R$$$-map calculated from $$$R_2$$$-map, $$$CBV$$$-map and $$$\delta\omega$$$-map (see Fig.2). The capillary radius is significantly increased in the tumor region (see Fig. 4).

Fig.4: Capillary radii distribution in healthy and tumor tissue. The capillary radii is significantly increased in the tumor region.

Proc. Intl. Soc. Mag. Reson. Med. 25 (2017)
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