Structual Neuroimaging Flashcards
(58 cards)
MRI vs fMRI
MRI looks at anatomy, while fMRI looks at the brain function
Magnetic fields
Magnets produce these magnetic fields
- attraction and repulsion of materials
- MRI machine can be dangerous if used incorrectly, due to the strong magnetic pull
- influence on nuclei -> nuclear magnetic resonance imaging
Nuclear magnetic resonance imaging NMR
Part of nuclei align with direction of the magnetic field
=/= radioactivity
- can cause nausea
- but no consequent short- or long-term illness
Hydrogen in fMRI
- human body is 55-78% water
- water molecules contain hydrogen atoms
- hydrogen atoms only contain one single proton
- atoms with uneven number of protons act as dipoles (even cancel eachother out and are not magentic)
Precess
Nuclei with odd number of protons/neutrons spin (precess)
- Larmor frequency
- depends upon magnetic field strength of the magnet
What causes Nuclear magnetic Resonance Imaging
If additional magnetic field oscillates with the Larmor frequency, nuclei absorb energy from the field
Static magnetic field
Atoms align with direction magnetic field
Oscillating magnetic field
If you add another magnetic field = radio frequency pulse (RF)
-> atoms spin/recess and get in phase (they will synchronise)
-> atoms flip and take direction of oscillating field
-> increase in energy state
When you remove RF pulse
- dephasing of atoms (spinning will be random
- realigning to static field (flip back) and this emits energy which you can see in the scan!
–> small signals over all the re-aligning nuclei integrate (stronger signal, when less dephasing)
Gradient of field strenght
- where does the signal come from?
Gradients are additional magnetic field over space: 3 different ones
–> they rely on the fact that the Larmor frequency depends on the field strenght
- if you add magnetic fields the Larmor will become larger
If magnetic field strength differs across space
- nuclei in different locations have a different Larmor frequency
- RP fulse only affets the nuclei with matching Larmor frequency
Three orthogonal gradients of field strength
- slice sletion gradient (at time of RF pulse Z)
- phase selection gradient (dephasing after RF pulse Y)
- frequency encoding gradient (at time of read out to signal X)
Slice selection gradient
- Applied during RF pulse
- RF pulse only affects nuclei that experience a total field strength with matching Larmor frequency
- Slice: volume of excited nuclei
- one slice per RF pulse for 2D, for full 3D there are as many RF pulses as there are slices
Interleaved slice acquisition
To minimize cumulative effects due to cross-slice excitation
- first all the odd slices, then the even slices for better results
Phase encoding gradient
- applied after RF pulse
- change spin resonance frequency of excited nuclei depending on their location in the gradient, causing dephasing
- when removed, resonance frequencies are the same again, but differenes in phase persist
- all nuclei at a certain position in the gradient have same phase, that phase is informative about position
Frequency encoding gradient
- applied during data acquisition
- = the read-out direction
- all nuclei at a certain position in gradient have same resonane frequency, thus frequency at read-out is informative about position
Summary of the gradients
- z-gradient (slice) cause slice selection
- y-gradient (phase) shows different phases
- x-gradient (frequency) shows the different frequencies
Pulse sequence
Succession of RF pulses and gradient changes
- pulse sequences differ in a number of ways
Pulse sequenes differ in a number of ways
- what happend prior to the RF pulse
- form and amplitude of the RF pulse
- direction and the amplitude of the gradients
- occurrence of one or multiple so-called gradient reversals
Voxels
Unit of space
- the shorter the time in which an image has to be taken, the lower the number of slices that can be imaged
–> the number of voxels per row/column in the slice relates back to number of steps of phase/frequency encoding gradient
How do these physical principles give rise to an image with anatomical structure?
Emitted signal decays over time and signal intensity depends upon sevel factors:
- density of H protons
- T1-recovery
- T2-decay
Factors are different in different tissues, resulting in signal contrast
Pulse sequence and parameter choice determine which factor has most weight
T1-recovery
Recovery of longitudinal orientation = spin-lattice relaxation
- realign with static magnetic field
T2-decay
Loss of transverse magnetization due to the loss in phase coherence = spon-spin interctions.
- Immediately after application of 90* RF pulse, transverse magnetization is maximized. It then begins to dephase due to natural interaction at anatomic or molecular levels. The signals from these dephasing protons begin to cancel out => MR signal decreases
T1-recovery time
= time it takes the longitudinal magnetization to grow back to 63% if its final value (all flipped back is 100%)
= spin-lattice relaxation time