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Gradient echo pulse sequences

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Title: Gradient echo pulse sequences


1
Gradient echo pulse sequences
  • Conventional gradient echo
  • Steady state Coherent gradient echo
  • Steady state Incoherent gradient echo
  • Steady state free precession
  • Ultra fast sequences
  • Echo planer imaging (EPI)

2
Gradient echo pulse sequences
  • Conventional gradient echo
  • Uses variable flip angles so that, TR and
    therefore the scan time, can be reduced without
    producing saturation.
  • A gradient instead of 180 rephasing RF pulse is
    used to rephase the FID.
  • The frequency encoding gradient is used for this
    purpose.
  • A gradient is quicker to apply than a 180 pulse
  • Therefore the minimum TE can be reduced.

3
  • Frequency encoding gradient is initially applied
    negatively to speed up the dephasing of the FID.
  • Then its polarity is reversed producing rephasing
    of the gradient echo.
  • Gradient does not compensate for magnetic field
    inhomogenities
  • So the resultant echo displays great deal of T2
    information
  • Used to acquire T2, T1, and proton density
    weighting
  • Allow for reduction in scan time as the TR is
    greatly reduced

4
Conventional gradient echo
TR
RF
RF
Echo
FID
FID
Frequency encode
rephase
dephase
TE
5
Uses of gradient echo
  • Used for single slice breath-hold acquisitions in
    the abdomen
  • Used for dynamic contrast enhancement
  • Used to produce angiographic type images, because
    the flowing nuclei which have been previously
    excited, always give a signal as gradient
    rephasing is not slice selective.

6
Manipulating Parameters
  • Flip angle and TR determines the degree of
    saturation and, therefore the T1 weighting.
  • For saturation flip angle should be large and TR
    short so that full recovery cannot occur.
  • To prevent saturation, flip angle should be small
    and the TR long enough to permit full recovery.
  • TE controls the amount of T2 dephasing
  • To minimize T2 Te should be short
  • To maximize T2 TE should be long.

7
Typical values
  • T1 weighting
  • Large flip angle 70 -110 degrees
  • Short TE 5-10 ms
  • Short TR less than 50 ms
  • Average scan time several seconds to minutes
  • T2 weighting
  • Small flip angle 5 -20 degrees
  • Long TE 15 -25 ms
  • Short TR enough for full recovery as flip angle
    is small
  • Scan time several seconds to minutes
  • Proton density weighting
  • Small flip angle 5 -20 degrees
  • Short TE 5 -10 ms
  • Short TR for full recovery as flip angle is small
  • Scan time several seconds to minutes

8
The steady state
  • This is a stage where the TR is shorter than the
    T1 and T2 times of the tissues.
  • There is no time for the transverse magnetization
    to decay, before the pulse sequence is repeated
  • There is coexistence of both longitudinal and
    transverse magnetization
  • The flip angle and TR maintain the steady state
    which holds the longitudinal and transverse
    components and the NMV steady during the data
    acquisition
  • Flip angles of 300 to 450 and TR of 20 to 50 ms
    achieves a steady state.

9
B0
Longitudinal component held steady
NMV held steady
Transverse component held steady
  • If steady state is maintained, the transverse
    component does not have time to decay during
    pulse sequence.
  • This transverse magnetization, produced as a
    result of previous excitations , is called the
    residual transverse magnetization(RTM)

10
  • The residual transverse magnetization (RTM)
    affects the contrast as it results in tissues
    with long T2 times , appearing bright on the
    image
  • Most gradient echo sequences use the steady
    state, as the shortest TR and scan times are
    achieved.
  • Gradient echo sequences are classified according
    to whether the residual transverse magnetization
    is in phase (coherent) or out of phase
    (incoherent).

11
Learning point
  • The steady state involves repeatedly applying RF
    pulses at TR less than the T1 and T2 of all
    tissues
  • This train of RF pulses generates two signals
  • A FID signal which occurs as a result of the
    withdrawal of the RF pulse and contains T2
    information
  • A spin echo whose peak occurs at the same time as
    an RF pulse

12
  • This happens because every RF pulse contains
    individual radio waves that have sufficient
    energy to rephase a previous FID
  • These radiowaves rephase the RTM left over from
    previous RF excitation pulses to form a spin
    echo.
  • This ocurs at exactly the same time as the next
    RF pulse as the RTM takes the same time to
    rephase as it took to dephase. Therfore when
    utilizing steady state , the TR TAU of the spin
    echo.

13
A FID and a spin echo occur at each RF pulse
RF pulse 2
Produces own FID and rephases FID of pulse 1
RF pulse 3
RF pulse 1
Spin echo
FID
FID
FID
dephasing
rephasing
TR
14
Summary
  • Any two RF pulses produce a spin echo.
  • The first RF pulse excites the nuclei regardless
    of its net amplitude
  • The second RF pulse rephases the FID resulting
    from the first.
  • The spin echoes produced are sometimes called
    Hahn or stimulated echoes.
  • This concept applies to all pulse sequences that
    use steady state.

15
GE-Coherent residual transverse magnetization
  • This pulse sequence uses a variable flip angle
    excitation pulse followed by gradient rephasing,
    to produce a gradient echo.
  • Steady state is maintained by selecting TR
    shorter than T1 and T2
  • There is therefore RTM left over when the next
    excitation pulse is applied.
  • The RTM is kept coherent by a process known as
    rewinding.

16
  • Rewinding is achieved by reversing the slope of
    the phase encoding gradient after readout.
  • This results in RTM rephasing, so that it is in
    phase at the beginning of the next repetition
  • This alows the RTM to build up so that tissues
    with a long T2 time produce a high signal.

17
Coherent gradient echo pulse sequence
TR
Rewinder gradient
Phase encode
readout
FID
echo
18
Sample image
  • T2 weighted image using a coherent gradient
    echo. TE 15 ms, TR 40 ms, flip 350, breath
    holding single slice obtained in 11s

19
Uses of coherent gradient echo
  • This pulse sequences produce T2 weighted images.
  • As fluid is bright they give an angiographic,
    myelographic or arthrographic effect.
  • Can be used to determine whether a vessel is
    patent, or whether an area contains fluid.
  • Can be acquired slice by slice, or in a 3D volume
    acquisition
  • As the TR is short, a sliice can be acquired in a
    single breath hold.

20
Parameters
  • To maintain the steady state
  • Flip angles 30 45
  • TR 20-50 ms
  • To maximize T2 long TE 15- 25 ms
  • Use gradient moment rephasing to accentuate T2
  • Average scan time
  • Seconds for single slice
  • 4-15 min for volumes
  • (to minimize T2 to produce T1 or proton density
    weighting TE should be the shortest possible)

21
Advantages Disadvantages
  • Very fast scans, breath holding possible
  • Very sensitive to flow so good for angiography
  • Can be acquired in a volume acquisition
  • Poor SNR in 2D acquisitions
  • Magnetic susceptibility increases
  • Loud gradient noise

22
Incoherent(spoiled) RTM
  • Pulse sequence that use incoherent RTM begin with
    a variable flip angle excitation pulse, and use
    gradient rephasing to produce agrdient echo.
  • The steady state is maintained so that RTM is
    left over from the previuos RF.
  • The RTM is spoiled so that its effect on image
    contrast is minimal.
  • There are two ways to achieve spoiling
  • Digitized RF spoiling
  • Gradient spoiling

23
RF spoiling
  • RF spoiling is achived by controling the phase of
    the digitised RF pulses that are transmitted.
  • The digitized RF is transmitted at a specific
    frequency phase
  • The resultant NMV and transverse component are
    fillped to a certain position in the transvere
    plane.
  • The receiver coil can lock onto the phase of the
    RF that has just being transmitted and receives
    only signal at that phase.
  • Transverse magnetization at other phases or
    positions in the transverse plane are not recived
    by the coil

24
  • Each RF is delivered at a different phase and the
    receiver coil is locked to recieve signal only at
    that phase
  • This process continues and the TRM which is at a
    different phase is ignored by the receiver coil.
  • So the effect of RTM on the image is eleminated.
  • T2 is therefore cannot predominate and T1 and
    proton density weighting prevails.

25
Uses
  • RF spoild GE pulse sequencs produce T1 or proton
    density weited images, although fluid may have a
    rather high signal due to gradient rephasing
  • Can be used for 2D and volume acquisition and as
    the TR is short the 2D acquisition can be used to
    acquire T1 weighted breath-hold images.
  • Demonstrate good T1 anatomy

26
Example for RF spoiled GE 5.21
  • T1/proton density weighted image using RF
    spoiling. TE 6 ms, TR 35 ms, flip 35, part of
    volume acqusition which took 7 minutes

27
Parameters
  • To maintain steady state
  • Flip angle 30-45
  • TR 20-50 ms
  • To maximise T1 short TE 5-10ms
  • Average scan time several seconds for single
    slice, 4-15 min for volumes
  • Advantages
  • Can be acquired in a volume or 2D
  • Breath holding possible
  • Good SNR and anatomical detail in volumes

28
Gradient spoiling
  • Gradient spoiling is the opposite of rewinding.
  • The slice select, phase encoding, and frequency
    encoding gradients can be used to dephase the
    RTM, so that it is incoherent at the beginning of
    the next repetition.
  • T2 effects are reduced
  • Uses and parameters are similar to those in RF
    spoiling.
  • Can be used to achieve T2 when the parameteres
    are similar to those in conventional GE.(because
    GS is less efficient than RF spoiling and moreT2
    information is present in the signal)

29
Steady state free prcession (SSFP)
  • Can be used to get shortest possible TR and scan
    time with steady state GE
  • Used to produce more T2 weighted images than
    conventional gradient echo sequences.
  • The pulse sequences used here help to obtain
    images that have a sufficiently long TE and less
    T2 when using steady state than other gradient
    echo pulse sequences.
  • This is achieved in the manner described below.

30
Composition of RF pulse
  • RF pulse contains radio waves of differing
    amplitudes. The magnetude of RF pulse is an
    average of these amlitudes. E.g.
  • 10 waves of amplitude of 100
  • 2 waves of amplitude of 300
  • 15 waves of amplitude of 600
  • 5 waves of amplitude of 1800
  • The average amplitude 19600/32 61.250

31
  • Therfore every RF pulse contains waves that on
    their own have sufficient magnitude to move
    magnetic moments within the NMV through 1800.
  • These radio waves are therefore able to rephase a
    FID.
  • In SSFP, the steady state can be maintained by
    using a flip angle between 300 and 450 with a TR
    of 20-50ms.
  • Every TR an excitation pulse is applied.
  • When the RF is switched off a FID is produced.

32
  • After the TR another excitation pulse is applied
    which also produces its own FID.
  • The radiowaves within it that have an amplitude
    of 180 rephase the FID from the previous pulse,
    and a spin echo is produced.
  • Each RF pulse therefore not only produces its own
    FID, but also rephases the FID produced from the
    previous excitation.
  • As nuclei take as long to rephase as they took to
    dephase, the echo from the first excitation pulse
    occurs at the same time as the third excitation
    pulse.
  • However this cannot be sampled, as RF cannot be
    transmitted and received at the same time.

33
  • To receive the spin echo, a rewinder gradient is
    used to speed up the rephasing process after the
    RF rephasing has begun.
  • The rewinding moves the echo so that it occurs
    before the next excitation pulse, rather than
    during it.
  • This way the resultant ehco can be received.
  • It demonstrate more true T2 weighting than
    conventional gradient echo sequences.
  • Because
  • The effective TE is now longer than the TR.
  • The rephasing is initiated by an RF pulse rather
    than a gradient so that more T2 and less T2
    information is present.

34
1
3
2
FID 1
Echo of FID 1
FID 3
FID 2
TE
TR
1
3
2
Rewinder gradient
FID 1
Echo of FID 1
Effective TE
35
Effective TE actual TE
  • Actual TE is the time between the echo and the
    next excitation pulse
  • Effective TE is the time from the echo to the
    excitation pulse that created its FID
  • Effective TE (2xTR) actual TE
  • If TR 50 ms, actual TE 10 ms
  • Then effective TE 90 ms

36
Uses of SSFP
  • Used to acquire images that demonstrate true T2
    weighting.
  • Especially useful in the brain and joints and on
    most systems can be used with both 2D and 3D
    volume acquisitions.

Effective TE 71 ms, TE 9ms, TR 40 ms, flip angle
350, volume scan time 9 minutes.
37
Parameters
  • To maintain steady state flip angle 30-45, TR
    20-50 ms
  • Actual TE affects the effective TE unless the
    system uses a fixed TE.
  • Average scan time 4-15 min volume acquisition
  • Some manufacturers suggest decreasing the
    effective TE to reduce magnetic susceptibility,
    and increasing the flip angle to create more
    transverse magnetisation which results in higher
    SNR

38
Comparison between Coherent, incoherent SSFP
RF pulse
RF pulse
RF pulse
FID spin echo
FID
FID
Spin echo
Gradient echo
Gradient echo
TE
TE
FID
TE
Spin echo moved away from RF pulse by rewinding
gradient
Coherent
Incoherent
SSFP
39
Ultra-fast sequences
  • Advances have been made in developing very fast
    pulse sequences.
  • Usually employ the coherent or incoherent
    gradient echo sequences.
  • The TE is significantly reduced by
  • Aplying only a portion of the RF exciation pulse.
  • Reading only a portion of the echo
  • TE kept to a minimum (2.5 3.0 ms)
  • TR and therefore the scan time is reduced.
  • TR as low as 10 ms is achieved and about 16
    slices can be achieved in a single breath hold.

40
  • Many ultra-fast sequences use extra pulses
    applied before the pulse sequences begins, to
    pre-magnetise the tissue.
  • This way certain contrast can be obtained.
  • Pre-magnetisation is achieved in the following
    manner.
  • Applying a 1800 pulse before the pulse sequence
    and a specified delay time similar to inversion
    recovery.
  • Applying a combination of 900/1800/900 pulses
    before the pulse sequence begins.

41
  • (first 90 pulse produces transverse
    magnetisation. 180 pulse rephases this, and at a
    specific time later second 90 pulse is applied.
    This drives the coherent transverse
    magnetisation into the longitudinal plane. It is
    available to be fliped when the pulse sequence
    begins. This is used to produce T2 contrast and
    is sometimes known as driven equilibrium)

42
Echo planer imaging(EPI)
  • Fills all the lines of k-space during one TR
  • Uses a single echo train
  • Multiple Echos are generated and each is phase
    encoded by a different slope of gradient to fill
    all the required lines of k space.
  • Echoes are generated either by 180 rephasing
    pulses or by gradients.
  • Gradients are much faster
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