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Imaging Sequences part II. Gradient Echo Spin Echo Fast Spin Echo Inversion Recovery. Spin Echo Refresher. 90 0 RF pulse followed by 180 0 RF pulse least artifact prone sequence moderately high SAR. Spin Echo. gradient. frequency encode. readout. RF pulse. RF pulse.
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Imaging Sequencespart II • Gradient Echo • Spin Echo • Fast Spin Echo • Inversion Recovery
Spin Echo Refresher • 900RF pulse followed by 1800 RF pulse • least artifact prone sequence • moderately high SAR
Spin Echo gradient frequency encode readout RF pulse RF pulse signal spin echo FID
Spin Echopulse timing RF slice phase readout echo signal TE
Spin Echo Contrast T1 weighted T2 weighted
Multi Echo Spin Echorationale • conventional imaging uses a multi-slice 2D technique • at a given TR time, number of slices depends on the TE time T2 weighted imaging: long TR long TE PD weighted imaging: long TR short TE
Multi Echo Spin Echo • designed to obtain simultaneously multiple echos • generally used for PD and T2 weighted imaging • no time penalty for first echo • inserted before second echo • can do multiple echos (usually 4) to calculate T2 relaxation values
Multi Echo Spin Echo gradient RF pulses RF pulse signal TE 1 TE 2
RF slice phase readout signal Multi EchoSpin Echopulse timing echo 1 echo 2
Spin Echo Contrast PD weighted T2 weighted
Multi Echo Spin Echo • Summary • simultaneously generates PD and T2 weighted images • no time penalty for acquisition of PD weighted image • no mis-registration between echos
Fast Spin Echo • Rationale • importance of T2 weighted images • most clinically useful • longest to acquire • lowest S/N • need for higher spatial resolution
Fast Spin Echohistorical perspective • faster T2 weighted imaging • gradient echo (T2*) • reduced data acquisition • “half-NEX”, “half-Fourier” imaging • rectangular FOV • S/N or spatial resolution penalty • altered flip angle SE imaging • “prise”, “thrift”
Fast Spin Echo • single most important time limiting factor is the acquisition of enough data to reconstruct an image • at a given image resolution, the number of phase encodings determines the imaging time
Fast Spin Echo • each phase encoding is obtained as a unique echo following a single excitation with a 90 degree RF pulse
….. TR echo echo ….. TR Spin Echopulse timing ….. phase encode n phase encode n+1 echo n echo n+1
Spin Echo Spin Echo Imaging Time = time-between-90-degrees times total-number-of-unique-echos times number-of-signal-averages
Spin Echoscan time • time-between-90-degrees = TR • total-number-of-unique-echos = phase encodings • number-of-averages = NEX, NSA
Fast Spin Echoimplementation • collect multiple echos per TR • similar to multi-echo SE • number of echos per TR referred to as the “echo train” • re-sort the data collection order to achieve the desired image contrast (effective TE time)
RF slice phase readout signal Multi EchoSpin Echopulse timing only 1 phase encode per TR echo 1 echo 2
RF slice phase readout signal FastSpin Echopulse timing multiple phase encodes per TR echo train
Fast Spin Echoscan time • time-between-90-degrees = TR • total-number-of-unique-echos = phase encodings • number-of-averages = NEX, NSA • echo-train-length = ETL
Fast Spin Echoadvantages • acquisition time reduced proportional to echo train length (ETL) • can trade-off some of the time savings to improve images • increased NEX • increased resolution
Fast Spin Echoadvantages • image contrast similar to SE • scan parameters • TR • TE • echo train length
Fast Spin Echodisadvantages • new hardware required • ear protection may be necessary • higher SAR • many 1800 flips closely spaced • motion sensitive
Fast Spin Echodisadvantages • reduced number of slices for equivalent TR SE scan • MT effects alter image contrast • TE time imprecise • image blurring may occur • fat remains relatively bright on long TR/long TE scans • “J-coupling”
FastSpin Echodisadvantages TE 20 Want: TR 3000, TE 80 Do: TR 3000, ET 4 20 msec IES TE 40 computer TE 60 TE 80 TE 70ef Get: TR 3000, TE 70ef
FastSpin Echodisadvantages • each echo “belongs” to a different TE image • combining the echos to form a single image creates artifacts • worse with shorter effective TE times
FastSpin Echoblurring SE TE 20 FSE TE 20
FastSpin Echolimitations • solutions: • use mainly for T2 weighted imaging • limit the ET length (~ 8) • many phase encodes (192 +)
FastSpin Echolimitations • solutions: • choose long TE times (> 100 msec) • choose long TR times (> 4000 msec) • increases fat-fluid contrast • for PD imaging, • use shorter echo trains (4) and wider receive bandwidths (32 kHz) • alternatively, use fatsat
FastSpin Echointerecho spacing • interecho spacing is the time between echos, ~ 16 msec minimum on current equipment • echo trains vary from 2 on up on current equipment • little signal is available with long echo train imaging
FastSpin Echointerecho spacing, example • 16 ETL, 16 msec IES results in echos at the following: • 16, 32, 48, 64, 80, 96, 112, 128, 144, 160, 176, 192, 208, 224, 240, 256 msec • last 5 or 6 echos have so little signal that there is little contribution to the final image
FastSpin Echointerecho spacing, example • time of last echo determines the number of slices per TR • long echo trains greatly reduce the number of slices per TR, even if the effective TE is short
FastSpin Echointerecho spacing • hardware upgrade (echo-planar capable) will decrease interecho spacing (6-8 msec) • better image quality for same echo train lengths • more slices per TR for identical echo train lengths
Fast Spin Echoconclusions • should be called “faster” spin echo • produces superior T2 weighted images in a shorter time than conventional SE • great innovation • artifact prone
Inversion Recovery • initially used to generate heavily T1 weighted images • popular in U.K. for brain imaging • 1800 inversion pulse followed by a spin echo or fast spin echo sequence
Inversion Recovery • three image parameters • TI • TR • TE
Inversion Recovery TR TI TE inversion recovery conventional SE or FSE sequence
z z 0 RF y x y x Initial 1800 Flipinversion 0 Before ML=M MXY=0 After ML=-M MXY=0 t=t0 t=t0+
z z y x y x T1 Relaxationrecovery After ML=-M MXY=0 t=t0+ t=TI
z z 0 RF y x y x 900 Flip 0 After MXY= ML Before ML=Msin() t=t0 t=t0+
z z z z y x y x y x y x Second 1800 Flip dephased rephased 1800 RF 900 RF t=0 t=TE/2 t=TE
STIR • Short time-to-inversion inversion recovery imaging • “fat nulling” • exploits the zero crossing effect of IR imaging • all signal is in XY plane after TI time and subsequent 900 pulse produces no signal
STIR • optimal inversion time for fat nulling dependent on T1 relaxation time
STIRadvantages • robust technique • works better than fat saturation over a large FOV (>30 cms) • better at lower field strengths • high visibility for fluid • long T1 bright on STIR • long T2 bright on STIR, given long enough TE
STIRdisadvantages • poor S/N • improved with multiple averages • FSE • improved with shorter TE times • incompatible with gadolinium • shorter T1 relaxation post-contrast
STIRdisadvantages • red marrow signal can obscure subtle edema • use TE=48 to knock signal down from marrow • modified IR • TE=70-100 • TI=110 @ 1.5T • excellent fluid sensitivity in soft tissues