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Questions and Answers
What occurs to the residual transverse magnetization in a Spoiled GRE?
What occurs to the residual transverse magnetization in a Spoiled GRE?
Which sequence of parameters would maximize T1 weighting in GRE imaging?
Which sequence of parameters would maximize T1 weighting in GRE imaging?
What disadvantage is associated with GRE images?
What disadvantage is associated with GRE images?
Which type of GRE is also known as incoherent GRE?
Which type of GRE is also known as incoherent GRE?
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How can PD images be produced in Spoiled GRE?
How can PD images be produced in Spoiled GRE?
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What is a benefit of using GRE imaging?
What is a benefit of using GRE imaging?
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What characterizes T2* decay in GRE imaging?
What characterizes T2* decay in GRE imaging?
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What technique is employed to spoil Mxy in GRE imaging?
What technique is employed to spoil Mxy in GRE imaging?
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What is a significant drawback of applying a 180 degree refocusing pulse in Spin Echo imaging?
What is a significant drawback of applying a 180 degree refocusing pulse in Spin Echo imaging?
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How does the application of multiple echoes affect scanning time in Fast Spin Echo imaging?
How does the application of multiple echoes affect scanning time in Fast Spin Echo imaging?
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Which combination of TR and TE maximizes T1-weighted imaging?
Which combination of TR and TE maximizes T1-weighted imaging?
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What is the echo train length (ETL) in relation to scanning time in Turbo Spin Echo imaging?
What is the echo train length (ETL) in relation to scanning time in Turbo Spin Echo imaging?
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Which of the following represents the typical value for a long TR in Spin Echo imaging?
Which of the following represents the typical value for a long TR in Spin Echo imaging?
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What effect does the 180o pulse have on the dephasing of the magnetization vector?
What effect does the 180o pulse have on the dephasing of the magnetization vector?
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During the TE/2 time, what happens to the magnetization vector?
During the TE/2 time, what happens to the magnetization vector?
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How do nuclei that precess at a frequency higher than ωL behave in the rotating frame?
How do nuclei that precess at a frequency higher than ωL behave in the rotating frame?
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What does the application of a 180o refocusing pulse do to the fan of magnetization vectors?
What does the application of a 180o refocusing pulse do to the fan of magnetization vectors?
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What is the phase relationship between the spin echo signal and the FID signal?
What is the phase relationship between the spin echo signal and the FID signal?
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Why is the amplitude of the spin echo smaller than that of the FID?
Why is the amplitude of the spin echo smaller than that of the FID?
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What does the term 'dephasing' refer to in the context of magnetization vectors?
What does the term 'dephasing' refer to in the context of magnetization vectors?
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What initial effect does a 90o pulse have on the magnetization vector Mz?
What initial effect does a 90o pulse have on the magnetization vector Mz?
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What is the purpose of adding a rewinder gradient in a coherent GRE sequence?
What is the purpose of adding a rewinder gradient in a coherent GRE sequence?
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How does the Inversion Recovery (IR) prepared-GRE contrast mechanism primarily work?
How does the Inversion Recovery (IR) prepared-GRE contrast mechanism primarily work?
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What happens to the transverse magnetization during a long TR in a GRE sequence?
What happens to the transverse magnetization during a long TR in a GRE sequence?
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What is the main characteristic of the Driven Equilibrium (DE) prepared-GRE technique?
What is the main characteristic of the Driven Equilibrium (DE) prepared-GRE technique?
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In what scenario is saturation most likely to occur during a fast GRE sequence?
In what scenario is saturation most likely to occur during a fast GRE sequence?
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What is the effect of using variable magnetic field gradients in a GRE sequence?
What is the effect of using variable magnetic field gradients in a GRE sequence?
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What initiates the Spin Echo (SE) process developed by Hahn?
What initiates the Spin Echo (SE) process developed by Hahn?
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What is the main purpose of using a 180° RF pulse in the Inversion Recovery technique?
What is the main purpose of using a 180° RF pulse in the Inversion Recovery technique?
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Which characteristic is true of the coherent GRE sequences?
Which characteristic is true of the coherent GRE sequences?
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In the DE-GRE technique, what does the TE/2 delay allow for?
In the DE-GRE technique, what does the TE/2 delay allow for?
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What happens to the resulting echoes in the Carr-Purcell sequence if the 180o refocusing pulse is not perfect?
What happens to the resulting echoes in the Carr-Purcell sequence if the 180o refocusing pulse is not perfect?
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In the Carr-Purcell Meiboom-Gill (CPMG) sequence, how does the RF carrier wave of the refocusing pulses compare to the 90o pulse?
In the Carr-Purcell Meiboom-Gill (CPMG) sequence, how does the RF carrier wave of the refocusing pulses compare to the 90o pulse?
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Which axis do spins flip about in the Carr-Purcell Meiboom-Gill sequence?
Which axis do spins flip about in the Carr-Purcell Meiboom-Gill sequence?
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What is the main advantage of the Carr-Purcell Meiboom-Gill sequence over the standard Carr-Purcell sequence?
What is the main advantage of the Carr-Purcell Meiboom-Gill sequence over the standard Carr-Purcell sequence?
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If a 180o refocusing pulse is applied improperly, what effect does it have on the decay of the echoes?
If a 180o refocusing pulse is applied improperly, what effect does it have on the decay of the echoes?
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In the Carr-Purcell sequence, what separation time is denoted as TE?
In the Carr-Purcell sequence, what separation time is denoted as TE?
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Which of the following accurately describes the behavior of echoes in the standard Carr-Purcell sequence?
Which of the following accurately describes the behavior of echoes in the standard Carr-Purcell sequence?
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What is the effect on magnetization if perfect 180o pulses are assumed in the CPMG sequence?
What is the effect on magnetization if perfect 180o pulses are assumed in the CPMG sequence?
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Which artifact can arise from cumulative errors in the 180o pulses of the Carr-Purcell sequence?
Which artifact can arise from cumulative errors in the 180o pulses of the Carr-Purcell sequence?
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Study Notes
Steady State Magnetization
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Residual transverse magnetization accumulates over multiple cycles until it reaches a steady state (Mss)
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In spin echo (SE) sequences, TR is long enough to allow complete dephasing of spins in the x-y plane, resulting in negligible x-y magnetization at the end of each cycle
Gradient Echo (GRE) Image Contrast
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GRE images can be optimized to highlight T1, T2*, or proton density (PD) by adjusting the pulse sequence parameters
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T1 weighting is achieved by using a large flip angle, intermediate TR, and short TE
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T2* weighting is maximized using a small flip angle, and long TR and TE
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PD weighting is achieved with a small flip angle, long TR, and short TE
Advantages and Disadvantages of GRE
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Advantages of GRE sequences include increased speed, sensitivity to magnetic susceptibility (useful for hemorrhage, functional imaging, and iron imaging), and capability to image flowing blood (magnetic resonance angiography, MRA)
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Disadvantages include decreased signal-to-noise ratio (SNR) due to smaller flip angles and short TRs and T2* decay, increased magnetic susceptibility artifact in regions like the paranasal sinuses or abdomen, and increased sensitivity to magnetic field inhomogeneity and intra-voxel dephasing
Coherent vs. Incoherent GRE
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The residual transverse magnetization can be either spoiled (destroyed) or cycled in GRE sequences
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Spoiled GRE, synonymous with incoherent GRE, destroys the residual transverse magnetization, leaving only longitudinal magnetization
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Non-spoiled GRE, known as coherent GRE, recycles the residual transverse magnetization, increasing its length from cycle to cycle
Incoherent (Spoiled) GRE
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Spoiling in incoherent GRE eliminates residual transverse magnetization, preventing the creation of T2 or T2* effects
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Long TR and large flip angles in incoherent GRE result in T1-weighted images
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With long TR and small flip angles, PD-weighted images are produced
Spoiling Methods
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RF spoiling offsets the phase of each successive RF pulse, causing cancellation of successive Mss vectors
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Variable magnetic field gradients, known as "crushers," are added with varying strengths between cycles
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Very long TRs completely dephase the Mss
Coherent GRE
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In coherent GRE, residual transverse magnetization is recycled, leading to an increasing Mss
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A rewinder gradient, opposite in polarity but similar in strength to the original phase encoding (PE) gradient, is used to counteract the phase shift introduced by the PE gradient
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This ensures no dephasing from previous PE gradients in subsequent cycles
Fast GRE Techniques
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Short TR and TE times are desirable for ultrafast GRE sequences
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Saturation of tissues with long T1 times, especially at high field strengths, can significantly reduce SNR
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To achieve high speed with preserving signal, two strategies are employed: Inversion Recovery (IR)-prepared GRE and Driven Equilibrium (DE)-prepared GRE
Inversion Recovery (IR)-prepared GRE
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A 180-degree RF pulse inverts the magnetization to -z before the GRE sequence begins
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An inversion time (TI) is introduced, allowing varying degrees of recovery back towards the +z axis for different tissues
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Tissues with shorter T1 times recover faster, leading to higher longitudinal magnetization at the start of the GRE sequence
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This technique introduces T1 contrast before the GRE sequence begins
Driven Equilibrium (DE)-prepared GRE
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A 90-degree RF pulse flips magnetization into the x-y plane
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A delay (TE/2) allows tissues to decay at different rates (T2*)
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A 180-degree pulse inverts the dephased spins along the -y axis
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After another TE/2 delay, the transverse vectors converge, but each tissue maintains its own vector length (tissues with shorter T2 times have smaller vectors)
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Another 90-degree RF pulse flips the vectors back to the +z axis
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All tissues are now aligned along +z but with different vector lengths, reflecting their T2 values
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A GRE sequence with a small flip angle excites the vectors, resulting in varying Mxy components and T2-weighted contrast
Spin Echo (SE)
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Introduced by Hahn in 1950, SE utilizes a 90-degree RF pulse followed by a 180-degree pulse for refocusing dephased spins
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The 180-degree pulse counteracts the effects of magnetic field inhomogeneity, leaving only signal degradation due to irreversible spin-spin (T2) relaxation
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The 180-degree pulse is often referred to as a "refocusing pulse"
Conventional (Hahn) SE
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A 90-degree RF pulse rotates magnetization from the +z axis to the y′ axis
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During TE/2, magnetic moments dephase due to spin-spin interactions and field inhomogeneity
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Nuclei experiencing higher magnetic fields precess faster, while those with lower fields precess slower, resulting in a fanning out of magnetization vectors
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A 180-degree refocusing pulse is applied along the x′ axis at time TE/2, rotating the fan 180 degrees around the x′ axis
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The dephased vectors converge along the -y′ axis at time TE after the 90-degree pulse
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The spin echo signal amplitude represents the remaining transverse magnetization after T2 relaxation, which is smaller than the initial FID signal
Carr-Purcell Sequence
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Multiple 180-degree refocusing pulses separate by TE are applied along the x′ axis, creating multiple echoes
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Echoes alternate between -y′ and y′, with decay reflecting true T2 if refocusing is perfect
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Imperfect 180-degree pulses cumulatively cause magnetization vectors to deviate from the transverse plane
Carr-Purcell Meiboom-Gill (CPMG) SE
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The RF carrier wave of the refocusing pulses is phase-shifted by π/2 relative to the 90-degree pulse in the CPMG modification
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This aligns the B1 field of the refocusing pulses along y′, while the 90-degree B1 remains along x′
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Spin flips occur around the y′ axis, resulting in all spin echoes converging along y′ with the same (positive) phase
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Perfect 180-degree refocusing is assumed for this description, and not all echoes can be utilized in practice
Important Notes about Spin Echo
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The 180-degree refocusing pulse eliminates the effect of T2*, preserving signal loss only due to irreversible T2 relaxation
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Drawbacks of the 180-degree pulse include increased scanning time due to longer TE and TR, and increased power deposition in the body
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Fast spin echo (FSE) or Turbo spin echo (TSE) sequences use multiple echoes to reduce scan time
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Echo train length (ETL) represents the number of echoes produced, with scan time reducing by this factor: Scan time (TSE) = Scan time (SE) / ETL
Image Contrast in Conventional SE
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T1 weighting is maximized using short TR and TE
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T2 weighting is maximized using long TR and TE
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PD weighting is achieved with long TR and short TE
Typical Values of Imaging Parameters for SE
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Long TR = 2000 ms
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Short TR = 300-700 ms
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Long TE = 60-80 ms
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Short TE = 10-25 ms
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Description
This quiz explores the concepts of steady-state magnetization and gradient echo (GRE) imaging techniques. It covers the factors influencing image contrast, including T1, T2*, and proton density weighting, as well as the advantages and disadvantages of GRE methods in MRI. Test your knowledge of these advanced imaging principles!