MEG, fMRI Flashcards
intro to fmri
- It works by placing a participant into a strong, static magnetic field, generated by a large superconducting electromagnet, cooled by liquid helium (needed to obtain superconductance)
- The field strength is usually 3 tesla (T) for experimental research (but there are also stronger magnets – University of Melbourne has a 7T scanner), or 1.5 T for
clinical purposes (the earth magnetic field is 65microtesla) - Participants are placed into the scanner, and their head is covered by a coil (RF coil)
- There are also gradient coils, which are used to modify the (otherwise ideally homogenous) magnetic field for short periods of time
safety of fmri
- Being exposed to a strong magnetic field is harmless to participants (some people do it hundreds of times)
- Moving in the field can make some people nauseous
- However, there is the danger of attracting magnetic objects (metal) which can be fatal – and since the field itself is invisible, it is easy to forget that it exists
participant view
- Participants can view experiments, which are controlled from outside the scanner room, via mirrors mounted on the head coil, or via goggles
- Responses can be given via scanner-compatible keys, joysticks, or a touchpad
- Participants’ head position is fixed to avoid any movement, which would distort the signal
- The head coil is used to send radio frequency (RF) pulses and also functions as a receiver for the incoming signal
Magnetic Resonance Imaging (MRI) – The Basics
In order to understand how functionalMRI works, we first need to get a basic understanding of how a structural image is acquired using MRI
- For this, we have to cover some of the basic physics of nuclear magnetic resonance (NMR), which is another word for the same method (but it does not refer to the use of any radioactive materials!)
- NMR refers to the anatomic nucleus, which contains protons and neutrons
- More than 70% of the human brain consists of water, which contains Hydrogen atoms (H+ protons)
- These can be thought as small bar magnets, “precessing” like a spinning top about an axis
Hydrogen in fmri
- The Hydrogen atoms are often simply referred to as protons, or “spins”
- Their “precessing” is often referred to as “spinning”
- The protons’ spin directions are initially random, but in a strong, externally applied magnetic field, like in the MRI scanner, they align parallel or anti-parallel to the magnetic field (often referred to as B0)
- Most protons align parallel to the B0 field
- However, they are not perfectly aligned – and they are also not static, but they still keep “precessing” in a random fashion
B0 field
- The B0 field is oriented into the direction of the Z-axis in the scanners coordinate system
- The precession frequency of the protons is also referred to as Larmor frequency
- Importantly, the precession frequency of protons depends on the strength of the magnetic field. This means, we know precisely the frequency with which they “spin” because we know how strong the magnetic field is.
- For simplicity, we can now imagine all protons being aligned with the B0 field, but they would all be in different positions in their precession (i.e. the phase in
which they spin is different) - However, as long as they are aligned in the direction of the B0 field we cannot measure a signal with our head coil, which surrounds the head
- The second problem is that the signal from each proton itself is tiny, and they are not precessing in phase (i.e. they are not in the same position at the same time)
radio frequency
In order to get a signal, we apply a radio frequency (RF) pulse perpendicular to magnetic field B0 using the head coil
- If the frequency of the RF pulse matches the precession (Larmor) frequency of the protons, it will affect these protons
effect of rf
- The first effect of the RF pulse is that all protons will start precessing (or spinning) in phase, meaning that their magnetisation will all point to same location in space at the same time
- This happens because the protons absorb energy from the RF pulse (which also heats up the tissue a bit)
- The second effect of the RF pulse is that the magnetisation vector (i.e. the net magnetisation that the protons have together) is tilted away from the Z-axis
- This means, the magnetisation is tilted from the longitudinal direction (of the field B0) into the transversal plane (the X-Y-plane)
receiving signal from fmri after rf
- The magnetisation vector now “rotates” around in the transversal plane where our head coil is placed
- The head coil will now receive this as a signal
- However, this signal is still rather meaningless for us, because it comes from the entire brain
- The trick is now to now switch off the RF pulse after which the transversal magnetisation decays very quickly because the protons emit the excess energy
- They also lose phase coherence very quickly, which makes the signal disappear
- Finally, the original longitudinal magnetisation will recover
T1 and T2
- The first consequence of switching off the RF pulse is that protons align again with the magnetic field, also referred to as longitudinal relaxation, spin-lattice relaxation (because it is due to an interaction of “spins”, the protons, and “lattice” the local environment), or T1 recovery
- T1 refers to a time constant of a function, indicating how long the recovery of the longitudinal magnetisation takes
- Importantly for us, this time constant is different for different tissue types
The second consequence of switching off the RF pulse is that the transversal magnetisation decays (which is an independent process), also referred to as transversal relaxation, spin-spin relaxation (because it is due to an interaction of “spins”, the protons, with other protons), or T2 decay - T2 is the time constant indicating how long the transversal decay takes
- T2 decay is much faster than T1 recovery, and again different for different tissues
Getting image from fmri via decay
- When the signal is measured during this phase of relaxation, different signals will be emitted from protons in different tissues
- Depending on when signals are measured, researchers can use T1 and T2 (and the density of protons) to get differently weighted images of the brain and clearly see the type of tissue (because the signal will be differently strong)
For this, different types of sequences (e.g., T1-weighted or T2-weighted) are used that are optimised to capture differences in signal, due to T1 recovery or T2 decay (or proton density) - Structural brain images depend on when signal is recorded during this process
Reconstructing brain images (slice 1)
- In order to get separate measurements from different locations in the brain, we first need to reconstruct where exactly the signal comes from
- For this, we use gradients created by the gradient coils
- Protons will absorb energy from RF pulses only when the frequency of the RF pulse matches the proton’s precession (also called “resonance”) frequency
- Thus, by causing the magnetic field to vary linearly, we can cause the resonance frequency to vary throughout the brain
- An RF pulse of a specific frequency will now only excite one slice of the brain –precisely the slice where the resonance frequency of the protons matches the frequency of the RF pulse
slice selecting gradient
- The first gradient we use is called slice selecting gradient
- It varies the gradient field along the Z-axis such that different slices are exposed to different field strengths
- A RF pulse can now be chosen to match precisely the precession frequency of protons in one “slice” of the brain
- This gradient is applied during the RF pulse
phase encoding gradient
- Now that we know the “slice” the signal comes from, the second gradient we use is called the phase encoding gradient
- It changes the precession (or, “spin resonance”) frequency of the excited protons depending on their location in the gradient, causing de-phasing
- When removed, the resonance frequencies are the same again, but the differences in phase persist – their phase is now informative about their position
- This gradient is applied after the RF pulse
frequency encoding gradient
- The third gradient is called to frequency encoding gradient, and it changes the magnetic field within the selected slice
- This happens during read-out of the signal
- Because all protons at a certain position in the gradient now have same resonance/precession frequency, the frequency at read-out is informative about their position
Gradient reversals
Gradient reversals are used to “un- do” the effects of the gradients
- The final signal consists of a series of “echos” elicited by the reversals (hence, sequences that use this trick are called gradient-eco, GE, sequences)
- Reversals of the RF pulse can also be used to create an echo (used in spin-echo sequences)
- This entire process, repeated for each slice, takes some time, meaning that it takes 1-3 seconds to measure the entire brain once
Other important parameters are in fmri
- In classical sequences, one RF pulse is used for each slice, meaning that the time it takes to measure the entire brain depends on the number of slices (called TR, time to repeat)
- The other important parameter is the echo time (TE), which is the interval between excitation and data acquisition
- Other important parameters are:
oThe slice thickness and gaps between them
oThe size of a measurement point, i.e. the “voxel”, the tree-dimensional pixel
oThe field of view (FOV), i.e. how many voxels we measure per slice
oThe number of slices we want
oThe orientation of the slices and read-out direction
the beginning Hemodynamic imaging
- fMRI does not measure neural activity directly but is a hemodynamic neuroimaging method
- Seiji Ogawa discovered in the early 1990s that large blood vessels cause “brighter areas” (i.e. better signal) in MRI scans
- Ogawa’s group (and another research team around Robert Turner) investigated this phenomenon in detail
- Ogawa changed the blood-oxygen level experimentally and found that this indeed impacts the signal
The science behind hemodynamic
- Local neural activity requires energy, which is generated in the brain in the form of adenosine triphosphate (ATP)
- To produce ATP, glucose is metabolised, for which oxygen is required
- Oxygen is constantly transported through the brain arteries and a network of arterioles (small arteries)
- In the capillaries, oxygen molecules are removed from hemoglobin (Hb), turning oxyhemoglobin into deoxyhemoglobin
- Deoxygenated hemoglobin is then transported away by the venules and the larger veins
What happens when there is local neural activity talk about blood oxy
- First, there is a slightly delayed increase of glucose and oxygen consumption
- This triggers an increase in cerebral blood flow (and blood volume) to supply more oxygen
- The consequence is a local increase in blood oxygenation
- The increase in blood oxygenation is much larger that the initial dip, meaning that shortly after the neural activity, there is an oversupply of oxygen in the blood
- The increase in blood oxygenation causes our signal to get better – this is the Blood Oxygen-Level Dependent (BOLD) signal we measure
- Oxygenated blood (oxyhemoglobin) is diamagnetic, enhancing the signal
Hemodynamic Response Function
HRF
- The change in signal is described by the Hemodynamic Response Function (HRF), which is similar (but not identical!) in different brain regions
- The peak of the HRF is reached 4-8 seconds after the neural activity occurred
- It takes the signal up to 16 seconds to go back to baseline levels
- If several neural events take place, their HRFs will add up linearly