This study demonstrates a new CSF flow imaging using multi spin echo acquisition cine imaging (MUSACI). MUSACI can obtain the high resolution CSF flow images more than the conventional phase contrast technique, moreover it is simple method because need not use a labeling pulse such as the time-SLIP technique. MUSACI can provide both morphological and physiologic information regarding CSF flow in a single scan.
The spin dispersion due to spin-phase effect is a change of the precession phase when a proton moves through a magnetic field gradient.4 In x-axis, the proton phase shift ($$$φ$$$) when the resonant frequency of the proton ($$$ω'$$$) moves at constant velocity ($$$v$$$) for time ($$$t$$$) within a gradient having constant magnitude ($$$G$$$) along the x-axis is given by;$$φ=∫ω'dt=∫γGvtdt=γGv∫tdt=(γGvt^2)/2$$
where $$$γ$$$ is the gyromagnetic ratio. This equation demonstrates that the proton phase shift influenced by a moving spin will be proportional to its velocity and the strength of the applied gradient, and the square of the length of time it moves within that gradient. The same respective equation (1) apply to the y- and z-axes.
The flow void phenomenon occurs in only the slice direction. The flow void appears in the condition that satisfy the following equation;$$v≥2d/TE$$
where $$$v$$$ is velocity, and $$$d$$$ is slice thickness. This equation indicates that the flow void readily appears at a higher velocity, however this appearance depends not only on velocity but also on TE. Thus, the use of multi spin echo acquisition allows for cine images of CSF flow because the flow void occurs at a different degree at each TE depending on its velocity.
All images were acquired on a 3T MR scanner (Ingenia 3.0T; Philips Healthcare) using a ds head coil and ds base coil. MUSACI images were acquired in the sagittal plane using 3D multi echo volume isotropic turbo spin echo acquisition (VISTA) with pulse gated. Turbo spin echo (TSE) factor and echo numbers were modified within one pulse wave at each volunteer and clinical case. Other scan parameters were as follows: TR/TE=2RR/7.3+echo number (80 ms step), FOV=240×240 mm2, matrix=416×411, slice thickness=1.2 mm (recon to 0.6 mm), slices=25, total scan time=approx. 5 min.
Figure 1 shows a series of midsagittal MUSACI images in a healthy volunteer. The anterograde CSF flow from the aqueduct to the fourth ventricle is observed on the images of TE 87.3 – 327.3 ms (arrow heads), and the retrograde flow from the aqueduct to the third ventricle is observed on the images of TE 327.3 – 647.3 ms (arrows). Moreover, MUSACI is able to image not only a midsagittal section but also the off-midline section for the foramen of Monro in the single 3D volume acquisition.
Figure 2 shows a series of MUSACI images at the section of the foramen of Monro. The retrograde CSF flow from the foramen of Monro to the lateral ventricle is observed on the images of TE 327.3 – 727.3 ms (arrows).
Figure 3 shows a series of midsagittal MUSACI images in a patient with germinoma in the pineal region and multiple disseminations in the lateral ventricles. There was no CSF flow in the third ventricle, aqueduct and the fourth ventricle because of the obstructions by the tumors (Fig. 3a). The MUSACI images acquired after chemoradiotherapy show the recovery of CSF flow from the aqueduct to the third ventricle or the fourth ventricle, and from the foramen of Monro to the third ventricle (Fig. 3b).
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