Table 1.
source | effect | consequence | severity | |
---|---|---|---|---|
RF transmit | 1. | motion of the object under investigation relative to the stationary, generally inhomogeneous transmit radiofrequency (TX-RF) fields |
contrast modulation |
low* |
2. | alteration of the TX-RF field(s) due to the coil loading changes and wave phenomena |
contrast modulation |
low* | |
3. | motion of the object with respect to the signal preparation or slice/slab RF excitation pulses |
contrast modulation |
high | |
RF receive | 4. | motion of the object relative to the stationary receiver coils and the corresponding radiofrequency fields (RX- RF), i.e. receiver coil sensitivities |
intensity modulation |
high |
5. | alteration of the spatial distribution of the RX-RF fields due to the coil loading changes, wave phenomena or motion of the coils in case of the flexible coils |
intensity modulation |
medium* | |
spatial encoding | 6. | motion of the object, including internal structures relative to the image encoding coordinates defined by the gradient pulses, receiver frequency and phase offsets |
partial-volume effect modulation |
high |
7. | motion of the object during the acquisition of multi- slice packages |
inconsistent 3D data |
medium | |
8. | local variations in spatial resolution corresponding to different positions due to the non-linearity of the spatial encoding fields |
modulation of distortions or blurring |
low† | |
Shimming & susceptibility |
9. | motion of the object-generated magnetic field inhomogeneities relative to the stationary B0 inhomogeneities and the stationary shim coils. |
B0 modulation | medium |
10. | alteration of the susceptibility-induced field distributions associated with a rotation of the object with respect to the B0 direction |
B0 modulation | medium* | |
local B0 modulation |
11. | alteration of the effective spatial encoding due to the changes in the local field inhomogeneities (motion to distortion interaction) |
modulation of distortions or blurring |
medium* |
12. | alterations due to local intra-voxel dephasing | intensity modulation |
medium* |
The consequence severity is based on the authors’ own experiences at 3T and may vary for different protocols and field strengths. In particular, severity tends to increase with higher main field strength for cells marked with asterisk (*), and also increases when a local head-only gradient coil is used for cells marked with dagger (†).