Title: Neuroimaging
1Neuroimaging
- Bart Krekelberg
- vision.rutgers.edu
- bart_at_rutgers.edu
Foundations II 21 March, 2006
2The neural basis of love
3Outline
- Positron Emission Tomography (PET)
- Physics
- Possibilities and Limitations
- Examples
- Magnetic Resonance Imaging (MRI)
- Physics
- Possibilities and limitations
- Practical MRI
4PET Physics
- Principle
- Find a molecule used in the brain.
- Make it radioactive.
- Put it in the brain
- Measure where the radiation comes from.
- Example
- Deoxyglucose
- Taken up by neurons just like glucose, but not
metabolized. - Add 18F to deoxyglucose and inject.
- Measure radiation.
?
e-
N
?
5PET Physics
6PET
- Limitations
- Need synchrotron to make tracer
- Need to inject tracer
- Poor temporal resolution
- Poor spatial resolution (3-9mm)
- Promise
- Baseline measurement possible
- Receptor-ligand specificity
7PET Examples
Blood entering the brain
8PET Examples
Dopamine production in Parkinsons patients
9MRI
10MRI Physics
A changing magnetic field causes an electrical
current at a distance
11Magnets in the brain
- Protons, neutrons, and electrons are all magnetic
- On average, there is no magnetic field
M00
12The brain in a (big) magnet
- Two things happen in a magnetic field
B0 M0
13Relaxation
14Relaxation
- T1
- Relaxation time constant
- For the protons in H20 1s
- Only 1 out 105 protons align with B0
- Per cubic centimeter M0 protons
- Difficult to measure
- M0ltlt B0
- M0 B0
- M0 constant after a few seconds
15Precession
- Two things happen in a magnetic field
B0 M0
16Mechanical Precession
Video UCSD Physics Program
https//physics-blog.ucsd.edu/weblog/physics2avide
o/ Lecture Angular Momentum Conservation
17Magnetic Precession
18Precession
19Precession
B0
Time
20Precession
- Mechanics strong force -gt fast precession
- Magnetism strong B0
- -gt fast precession
- Larmor Equation ? ?B0
- ? Larmor frequency
- ? gyromagnetic ratio
- 42MHz/T for protons (1H)
- 11MHz/T for 13C
- 176GHz/T for electrons (e-)
21A Proton in a Strong Magnet
22Transverse Magnetization
- Mt is orthogonal to B0
- Mt changes -gt causes an electrical field
- But, Mt lasts only seconds (T1)
- Can we flip the magnets?
23Flipping with a static field
24Flipping with a static field
- Another huge magnet?
- Relaxation in B1 direction T1
25Flipping with a dynamic field
26Mechanical Resonance
27Magnetic Resonance
B1
Precession
Time
28The Flip Angle
29The B1 field
- Even a small B1 can produce a large flip angle in
a short time if it oscillates at the Larmor
frequency - A large B1 at the wrong frequency does nothing
- Larmor 120MHz for protons in 3T -gt Radio
Frequency Pulse - After the RF pulse we have a magnetic field that
is - changing (precessing)
- macroscopic (in phase)
- transverse (flip angle)
- This causes a measurable electrical current at a
distance.
30The basic MR experiment
31Density weighting
- Flip, then measure
- Insensitive to relaxation times (no time)
- Sensitive to proton density
32The basic MR experiment
Single proton
33Dephasing T2 relaxation
- Random events cause small changes in the magnetic
field - Changes in the magnetic field change the
precession speed (Larmor) - Some protons speed up, others slow down and they
become out-of-phase - The (small) currents caused by these protons no
longer sum the signal decays.
34T2 transverse relaxation time
- Depends on tissue type
- White matter 70 ms
- Gray matter 90 ms
- CSF 400 ms
- T2 ltlt T1
- Measure the signal 200 ms after the RF pulse.
- White matter e-200/70 5
- Gray matter e-200/90 10
- CSF e-200/400 60
35What about T1?
M0,max
Time
36T1-weighted images
- If TR gtgt T1 then T1 has no influence
- Density weighted image
- T1 at 1.5T
- Gray matter 900 ms
- White matter 700 ms
- CSF 4000 ms
- TR 400ms, measure soon after RF pulse (ltltT2)
37MR Imaging
- Tissue Parameters
- T1
- T2 (T2)
- Proton density
- Scan parameters
- TR
- Measurement time after RF Pulse (TE)
38But
- How do I make an image?
- How does this relate to neural activity?
39Making an image
- Slice selection with a gradient field
z
- Set a z-gradient
- Choose the frequency of the RF pulse
- Switch of the z-gradient
40Making an image
- Frequency encoding with a gradient field
Bx
0
x
Faster precession fast changing signal
Slower precession slow changing signal
- When measuring the signal, set a gradient
- Measure only fast signals -gt back of head
- Measure only slow signals -gt front of head
41Making an image
- Phase encoding with a gradient field
By
0
y
- After the RF pulse, set a gradient for a brief
time - Measure the signal
- The phase of the signal depends on the y-position
sin(y) - Repeat, with ever stronger gradient
- The signal sin(2y), sin(3y), sin(4y)
- Signals that change rapidly with the repeat
number have large y - Signals that change slowly with the repeat number
have small y
42Making an Image
- Magnetic Field Gradients for
- Slice selection
- Frequency encoding
- Phase encoding
43Neural activity
- Neural activity increases T2
Time
Measure here
44Neural activity
2005 Monkey, 7T
1992 Human, 1.5T
45Neural activity
Oxyhemoglobin (Hb02)
Deoxy-hemoglobin (Hb)
46The BOLD Signal
- Blood Oxygen Level Dependent
- Hb is paramagnetic and reduces T2
- Active neurons use the O2 from HbO2
- Neural activity increases Hb and therefore
reduces T2 - Didnt I say activity increases T2 before??
- The vascular system overcompensates for the
increased O2 consumption by increasing blood flow
and volume. - The net effect is that activity leads to a
decrease in Hb and therefore an increase in T2 -
47The BOLD signal
- Limitations
- It takes 2-3 seconds before the HbO2
overcompensation is maximal. - Neurons draw HbO2 from a fairly wide region.
- Cannot distinguish between excitatory or
inhibitory activity (or anything else that uses
O2). - Promise
- Non-invasive, works in humans
48MRI in practice
49The MR room
50Scanner Internals
51The Magnet
- Goal align the protons
- Coils
- Super conductance Helium
- 1.5T, 3T, 7T (Earth magnetic field 0.0005T)
- Side Effects (FDA lt8T, neonates lt4T )
- Nausea
- Vertigo
- Tingling
- Headache
- Pain in tooth fillings
52Not harmful?
53The Gradient Coils
- Goal
- Slice selection
- Frequency encoding
- Phase encoding
- Side Effects
- Induced currents (dynamo small)
- Nerve stimulation
- Phosphenes
- Acoustic Noise
54The RF Coil
- Goal
- Turn longitudinal magnetization into transverse
magnetization - Measure the signal generated by the precessing
spins. - Side Effects
- Induced currents Specific Absorption Rate (SAR)
limits - Heating avoid loops.
55Links to more information
- Handouts
- Principles of Neural Science Eric Kandel , James
Schwartz, Thomas Jessel Pages 366-380 - Introduction to Functional Magnetic Resonance
Imaging Principles and Techniques Richard B.
Buxton Chapter 4 (Pages 64-85) - Webpages with additional material and sources for
these slides - Jody Culha ms fMRI for Newbies
http//www.ssc.uwo.ca/Jody_web/fmri4newbies.htm - BrainTutor Learn about the human brain
http//www.brainvoyager.com/BrainTutor.html