EPI – Echo Planar Imaging Joakim Rydell
Echo Planar Imaging Like ordinary MR, but faster Ordinary MR: approximately one minute EPI: less than one second The Nobel Prize in Medicine 2003 Lauterbur (MR) Mansfield (EPI)
Repetition, k-space Fourier transform of image Traversed using magnetic field gradients
Repetition, pulse sequence Slice selection Phase encoding Frequency encoding
Introducing EPI Acquire all rows in k- space with just one excitation EPI Ordinary MR
EPI – The Movie
Going even faster – Partial Fourier Real image hermitian symmetric k-space Acquire half of k-space, compute the rest Not always as good as it seems...
Partial Fourier, drawbacks Phase errors Slowly varying Approximately 65 % of k-space required SNR decrease Full k-space acquisition gives sqrt(2) SNR improvement
Why use ordinary MR? Signal decay Low SNR N/2 ghosting Geometric distortion dB/dt
Signal decay Long readout period Weak signal near end of acquisition Blurring in phase- encoding direction
Low SNR Fast acquisition Less averaging Noisy images
N/2 ghosting Alternating acqusition directions Shifted sampling positions N/2 ghosting Reference scans
Geometric distortion Low bandwidth/pixel Pixels shifted in phase encoding direction Field maps
dB/dt Fast gradient switching induces eddy currents, causing field inhomogenity Rapid changes in the magnetic field can cause peripheral nerve stimulation
k-space trajectories Cartesian Blurring N/2 ghosting High dB/dt Spiral Non-uniform sampling Cartesian spiral
Ramp sampling Sampling on gradient ramps Non-uniform sampling In time In k-space
Multishot Both EPI and ordinary imaging Collect several rows per excitation Alignment difficulties
Applications Cardiac imaging fMRI...
EVI – Echo Volumar Imaging 3D EPI Acquire a full volume with just one excitation Not quite possible yet