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Achieva 1.5 t mri scanners

Manufactured by Philips

The Philips Achieva 1.5 T MRI scanner is a magnetic resonance imaging system capable of providing high-quality images. It operates at a field strength of 1.5 Tesla and is designed for clinical use.

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2 protocols using achieva 1.5 t mri scanners

1

Prostate MRI Radiomics Protocol

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All of the patients received a high-resolution T2-weighted MRI scan in the pelvic region at diagnosis. The images were taken using Philips Medical Systems Achieva 1.5 T MRI scanners with a 2 mm slice thickness. Using Velocity software (Varian Medical Systems, Palo Alto, CA, USA), each MRI scan was manually contoured on two separate ROIs: the prostate gland and the peripheral zone of the prostate. The whole prostate gland is the most common region reviewed by radiologists and also easy to contour for future studies, while the peripheral zone is where over 90% of prostate cancers develop [30 (link)]. Figure 1 shows the created contours on two example patients, with the prostate gland outlined in blue and its peripheral region outlined in red.
All of the images and segmented ROIs were then sent to 3D-Slicer v4.10 for image processing and radiomic feature extraction [31 (link),32 (link)]. To avoid bias field distortions and data heterogeneity bias, a bias field correction using N4 and an image normalization using histogram matching were performed on all images [33 (link)].
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2

Neuroimaging Protocol for Osaki-Tajiri and Kurihara

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Brain scans for the Osaki-Tajiri and Kurihara projects were acquired on Achieva 1.5T MRI scanners (Philips Medical Systems, Best, Netherlands) by using a sagittal 3D T1-weighted turbo field echo (3D T1-TFE) sequence and an axial 2D FLAIR sequence with eight-channel phased array head coils. The acquisition parameters for the 3D T1-TFE sequence were as follows: repetition time (TR), 9.3 ms; echo time (TE), 4.6 ms; flip angle (FA), 8° for Osaki-Tajiri and 10° for Kurihara; field of view (FOV), 240 mm; and in-plane resolution, 256 × 256 (0.94 × 0.94 mm) with a slice thickness of 1 mm and no intersection gap. Axial FLAIR images were scanned with the following parameters: TR/TE/inversion time (TI), 11000/140/2800 ms for Osaki-Tajiri and 8000/120/2500 ms for Kurihara; FA, 90°; FOV, 230 mm; in-plane resolution, 512 × 512 (0.45 × 0.45 mm); and slice thickness/intersection gap, 5/0.5 mm for Osaki-Tajiri and 6/1 mm for Kurihara.
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