Proton nuclear magnetic resonance images (proton MRI) are functions of not only proton density (¿), spin lattice relaxation time (T1), and spin-spin relaxation time (T2) but also MRI scan parameters, so the images differ for different pulse sequences and scan parameters. Systematic measuring errors also vary depending on the type of pulse sequence and the scan parameters. "Pure," objective, T1, T2, and proton density images can be computed from several different Proton MRI, however, systematic measuring errors can cause large deviations between "pure" images obtained using different methods. We tested several scan sequences, and investigated methods to improve the resolution and reduce the errors over the range of T1, T2, and proton density values encountered in representative human tissues. We found that, for given scan time, the combination of inversion recovery 3 spin echo (IR3SE) and saturation recovery 4 spin echo (SR4SE) sequences gave more accurate computed images than other comparable methods tested. It follows, then, that adopting such a sequence as "standard" allows meaningful comparison of clinical results obtained by different researchers.
[1]
A. J. Shaka,et al.
Composite pulses with dual compensation
,
1983
.
[2]
A New Pulse Sequence for "Fast Recovery" Fast-Scan NMR Imaging
,
1984,
IEEE Transactions on Medical Imaging.
[3]
B R Rosen,et al.
Spin lattice relaxation time measurements in two-dimensional nuclear magnetic resonance imaging: corrections for plane selection and pulse sequence.
,
1984,
Journal of computer assisted tomography.
[4]
J N Lee,et al.
Automated MR image synthesis: feasibility studies.
,
1984,
Radiology.
[5]
W. Edelstein,et al.
Calculated T1 images derived from a partial saturation-inversion recovery pulse sequence with adiabatic fast passage.
,
1985,
Magnetic resonance imaging.
[6]
Ingwer C. Carlsen,et al.
Real-Time Interactive NMR Image Synthesis
,
1985,
IEEE Transactions on Medical Imaging.