Ma. Moerland et al., ANALYSIS AND CORRECTION OF GEOMETRIC DISTORTIONS IN 1.5-T MAGNETIC-RESONANCE IMAGES FOR USE IN RADIOTHERAPY TREATMENT PLANNING, Physics in medicine and biology, 40(10), 1995, pp. 1651-1664
The aim of this study is to investigate and correct for machine- and o
bject-related distortions in magnetic resonance images for use in radi
otherapy treatment planning. Patients with brain tumours underwent mag
netic resonance imaging (MRI) in the radiotherapy position with the he
ad fixed by a plastic cast in a Perspex localization frame. The imagin
g experiments were performed on a 1.5 T whole body MRI scanner with 3
mT m(-1) maximum gradient capability. Image distortions, caused by sta
tic magnetic field inhomogeneity, were studied by varying the directio
n of the read-out gradient. For purposes of accuracy assessment, exter
nal and internal landmarks were indicated. Tubes attached to the cast
and in the localization frame served as external landmarks. In the mid
sagittal plane the brain-sinus sphenoidalis interface, the pituitary g
land-sinus sphenoidalis interface, the sphenoid bone and the corpora o
f the cervical vertebra served as internal landmarks. Landmark displac
ements as observed in the reversed read-out gradient experiments were
analysed with respect to the contributions of machine-related static m
agnetic field inhomogeneity and susceptibility and chemical shift arti
facts. The machine-related static magnetic field inhomogeneity in the
midsagittal plane was determined from measurements on a grid phantom.
Distortions due to chemical shift effects were estimated for bone marr
ow containing structures such as the sphenoid bone and the corpora of
the cervical vertebra using the values obtained from the literature. S
usceptibility-induced magnetic field perturbations are caused by the p
atient and the localization frame. Magnetic field perturbations were c
alculated for a typical patient dataset. The midsagittal head image wa
s converted into a susceptibility distribution by segmenting the image
into water-equivalent tissues and air; also the Perspex localization
frame was included in the susceptibility distribution. Given the susce
ptibility distribution, the magnetic field was calculated by numerical
ly solving the Maxwell equations for a magnetostatic held. Results wer
e shown as magnetic field perturbations and corresponding spatial dist
ortions of internal and external landmarks. The midsagittal head image
s were corrected for the machine imperfections (gradient non-linearity
and static magnetic field inhomogeneity). The locations of the extern
al landmarks in the frame were also corrected for susceptibility artif
acts. The efficacy of the corrections was evaluated for these external
landmarks in the localization frame with known geometry. In this stud
y at 1.5 T with read-out gradient strength of 3 mT m(-1), machine-rela
ted, chemical shift and susceptibility-induced static magnetic field i
nhomogeneity were of the same order, resulting in spatial distortions
between -2 and 2 mm with only negative values for the chemical shift e
ffect. Both the patient and the localization frame proved to perturb t
he magnetic field. The field perturbations were shown to be additive.
In total, static magnetic held inhomogeneity led to spatial distortion
s ranging from -2 to 4 mm in the direction of the read-out gradient. N
on-linearity of the gradients resulted in spatial distortions ranging
from -3.5 to 0.5 mm. After correction for the machine imperfections an
d susceptibility artifacts, the geometric accuracy of the landmarks in
the localization frame was better than 1.3 mm.