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MRI Physics: Spin Echo Pulse Sequences

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MRI Physics: Spin Echo Pulse Sequences Nicole Seiberlich Associate Professor, Radiology Co-Director of MIITT
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Page 1: MRI Physics: Spin Echo Pulse Sequences

MRI Physics:

Spin Echo Pulse Sequences

Nicole SeiberlichAssociate Professor, Radiology

Co-Director of MIITT

Page 2: MRI Physics: Spin Echo Pulse Sequences

Pulse Sequences: What do we use?

• Spin Echo

• Gradient EchoSpoiled Gradient EchoBalanced Gradient Echo

• SE / GE + Prep Pulses to boost contrast

Page 3: MRI Physics: Spin Echo Pulse Sequences

Spin Echo Pulse Sequence Diagram

TE

90◦ TR

echo

RF

acquisition

signal

TE/2

180◦

Page 4: MRI Physics: Spin Echo Pulse Sequences

Spin Echo MRI Contrast

[ ] 2/1/1 TTETTRo eeSS ---=

• TR à very long, then expà 0 Image is T2-weighted• TR à medium Image is T1-weighted• TR à 0 No signal

• TE à 0, then expà 1 Image is T1-weighted• TE à medium Image is T2-weighted• TE à very long No signal

Page 5: MRI Physics: Spin Echo Pulse Sequences

Spin Echo MR Images

Conventional contrast:

T1-weightedTR=500msTE=15ms

TR=4000msTE=15ms

TR=4000msTE=90ms

PD-weighted T2-weighted

Page 6: MRI Physics: Spin Echo Pulse Sequences

Spin Echo MRI is SLOOOOW

Spin-Echo~ minutes

Single-Shot EPI~ 0.1sec

Page 7: MRI Physics: Spin Echo Pulse Sequences

Spin Echo MRI is just very slow

• SLOWÞ Long scan durationScan time = TR x Ny ( x Nave)Typically TR in range 300ms ® 4000msGiven TR = 2000ms, Matrix = 256, Nave = 1

Scan time = 2000ms x 256 = 512sec = 8.6 minFor ”pure” T2 or PD weighting, TR > 5xT1 to minimize T1 effectsTR ~ 5000ms Þ 21 min for 256 matrix size

• Long scan time Þ artifacts due to motion

Page 8: MRI Physics: Spin Echo Pulse Sequences

Spin Echo Variant: Multiecho SE MRISignal

T2 relaxation

T2*

RF/Data Data Data

180o 180o 180o

90o

Page 9: MRI Physics: Spin Echo Pulse Sequences

Spin Echo Variant: Multiecho SE MRI

• Turbo Spin Echo (TSE)• Fast Spin Echo (FSE)

• Way faster than Spin EchoTurbo Factor/Echo Train Lengthà6Number of echoes collectedFactor by which scan is accelerated

Collected in 1 TR

Page 10: MRI Physics: Spin Echo Pulse Sequences

T2 Contrast Determined by Center of k-Space

Center Echo

TEeff

Page 11: MRI Physics: Spin Echo Pulse Sequences

Potential Disadvantages of TSE

• Complex T2 weighting (not all of image data is weighted the same way)

• Some “blur” or “edge-enhancement” occurs since T2-decay and spatial encoding coincide

• Fat exceptionally bright due to funny physics (J-coupling effect)

• High RF power deposited in tissue (high SAR) due to multiple 180°pulsesà May not be possible at 3T

Page 12: MRI Physics: Spin Echo Pulse Sequences

FSE / TSE MRI - Examples

T2wt FSE / TSETR=3600ms TE=80ms

ETL = 16T2wt FLAIR FSE / TSE

TR=11000 TE=125 TI=2800ETL = 27 IR-prep T1wt FSE / TSE

TR=2100 TE=20 TI=800ETL = 7

Page 13: MRI Physics: Spin Echo Pulse Sequences

FSE MRI Single-Shot FSE(ETL~64-128)

Breathhold T2w MRCP

Page 14: MRI Physics: Spin Echo Pulse Sequences

Spin Echo Pulse Sequences

• TR controls T1 weighting• TE controls T2 weighting• Can be combined with “preparation pulses”• Lack of T2*à fewer distortions/artifacts than other sequences• Often used in multi-echo format

• Conventional Spin Echo is VERY Slow• Multi-echo à High SAR due to many 180◦ pulses• Multi-slice à Dead time during TR used to scan additional slices

Page 15: MRI Physics: Spin Echo Pulse Sequences

MRI Physics:

Gradient Echo Pulse Sequences

Nicole SeiberlichAssociate Professor, Radiology

Co-Director of MIITT

Page 16: MRI Physics: Spin Echo Pulse Sequences

Gradient Recalled Echo (GRE) Pulse Sequence

TE

α α

TR

echo

RF

slice selection

phase encoding

frequency encoding

acquisition

signal

1) No 180 pulse 2) Flip angle less than 90 3) Additional gradient to make echoCompared to Spin Echo:

Page 17: MRI Physics: Spin Echo Pulse Sequences

T2* Relaxation Dephases Magnetization (signal loss)

Page 18: MRI Physics: Spin Echo Pulse Sequences

T2* Decay of signal following RF pulse

Sign

alTime (~ 2 - 30msec)

Gradient EchoT2*

gradient acts to destroy Mxy gradient reversal

acts to rebuild Mxy

Page 19: MRI Physics: Spin Echo Pulse Sequences

GRE Sequence

• T2* Weighting, not T2 (but can be altered)

• Use of small flip angles

• à significant residual Mz after RF pulse

à data can be collected at much shorter times

TR (200ms ® 2ms) and TE (50ms ® 0.5ms)

• Signal moves into a “steady state” of low SNR

Page 20: MRI Physics: Spin Echo Pulse Sequences

Very Short TR, Short TE, small flip angle (GRE)

Page 21: MRI Physics: Spin Echo Pulse Sequences

Sub-Classes of GRE

Many sub-classes GRE sequences with very different contrast behavior

• FLASH: Fast Low-Angle Shot (multiple versions Siemens)• GRASS: Gradient Recalled Acquisition in the Steady State (General Electric)• FFE: Fast Field Echo (Philips)• FISP: Fast Imaging w/ Steady Precession (Siemens)• TrueFISP (Siemens); FIESTA (GE); Balanced FFE (Philips)• SPGR: Spoiled GRASS; Spoiled FLASH; T1-FFE• SSFP: Steady-state free precession• many others …

Page 22: MRI Physics: Spin Echo Pulse Sequences

Sub-Classes of Gradient Echo Sequences

SEQUENCE TYPE GE PHILIPS SIEMENS Gradient Echo GRE FFE GRE Coherent Gradient Echo GRASS FE FISP Spoiled Gradient Echo SPGR T1-FFE FLASH Steady-State Free Precession

SSFP T2-FFE PSIF

True FISP FIESTA Balanced-FFE b-FFE

TrueFISP

Fast Gradient Echo Fast GRE; Fast SPGR

Turbo-FFE; TFE

TurboFLASH

Fast T1wt 3D GRE 3D FGRE; 3D FSPGR;

LAVA

3D TFE; THRIVE

MPRAGE; VIBE

Can have very different contrast behavior (depending on steady-state and sequence settings)

Page 23: MRI Physics: Spin Echo Pulse Sequences

Spoiled Gradient Echo MRI (SPGR and FLASH)

[ ] *2/1/

1/

)cos(1)sin(1 TTE

TTR

TTR

ee

eSoS -

-

-

--

=q

q

TR=7 TE=min

0

0 30 60 90Flip Angle (degrees)

SPG

R S

igna

l

T1=50 (1pass Gd in blood)

T1=270 (fat)

T1=600 (liver)

TR=150 TE=min

0

0 30 60 90Flip Angle (degrees)

SPG

R S

igna

l

T1=50 (1pass Gd in blood)

T1=270 (fat)

T1=600 (liver)

Control T1 contrast by flip angle and TR (min TE):

Page 24: MRI Physics: Spin Echo Pulse Sequences

Two options for T1-weighted Imaging (+Gd)

2D Spin-EchoTR=500ms TE=10ms

3D Spoiled GRE (SPGR)TR=10ms TE=6ms Flip = 8o

256 x 0.5 s2.1 min

256 x 0.01 s2.5 sec

3D256 x 64 x 10ms2.67min

Page 25: MRI Physics: Spin Echo Pulse Sequences

(Spoiled) GREmore sensitive to local

distortion and signal loss due to T2* sensitivity

Spin Echoless sensitive to local

distortion and signal loss

Spin Echo vs GRE: Local Signal Dephasing

metal implant metal implant

Page 26: MRI Physics: Spin Echo Pulse Sequences

Spin-Echo vs EPI: Geometric Distortion and Local Signal Dephasing

SS GRESE SS SE

Page 27: MRI Physics: Spin Echo Pulse Sequences

Spoiled Gradient Echo

• Very fast, primarily T1-weighted imaging

à Contrast controlled by FA and TR

• Enables full 3D imaging

à Great for dynamic imaging or for breathhold scans

• Slower but can be used for T2*-weighted imaging

• Low SNR (can be boosted by using 3D acquisition)

• Signal loss/Distortion around sources of magnetic field inhomogeneities

Page 28: MRI Physics: Spin Echo Pulse Sequences

Fully Balanced Gradient Echo MRI (bSSFP, TrueFISP, FIESTA, bFFE)

)cos()]2/1(1[)]2/1(1[)sin(

qq

TTTTSo

S-++

=

00 30 60 90

True

FIS

P Si

gnal

Flip angle (degrees)

T1 = 2000; T2 = 1000 (eg. CSF & blood)

T1 = 800; T2 = 80 (eg. tissue)

NO dependence on TR or TEBUTTE must be TR/2TR short due to “banding artifacts” from

magnetic field inhomogeneities

T2/T1 contrast

Page 29: MRI Physics: Spin Echo Pulse Sequences

T1-FFE vs Balanced-FFESingle-shot locator scans

TR = 8msTE = 2.3msFlip = 15o

“T1-enhanced” (Spoiled)

TR = 3msTE = 1.5msFlip = 60o

“Fully Balanced”

Page 30: MRI Physics: Spin Echo Pulse Sequences

3D bFFE

TR=6ms, TE=3ms, flip=45,0.5mm slices

Note – thin black bands due to Bo inhomogeneity

Examples Balanced FFE / FIESTA / TrueFISP

Page 31: MRI Physics: Spin Echo Pulse Sequences

Balanced Gradient Echo

• bSSFP, FIESTA, TrueFISP, bFFE

• Very fast, T2/T1 contrast

à Contrast not significantly affected by TR, TE, even flip angle

• High SNR

• TE = TR/2

• Short TR best (2-5 ms)

à Longer TR leads to “banding” artifacts near at field inhomogeneities


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