Estimating Oxygen Saturation of Blood in Vivo with MR

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Transcript Estimating Oxygen Saturation of Blood in Vivo with MR

Mark Elliott, PhD
Associate Director of CMROI,
Department of Radiology,
University of Pennsylvania School of Medicine, Philadelphia, PA
Overview



CMROI
Mechanisms of functional imaging with NIR
light
Methodology of fNIR
Comparison with and without Difuse Optical
Tomography (DOT)
Slide 2
Methods for Imaging Neural
Activity
metabolic response
electrical activity
- excitatory
- inhibitory
- soma action potential
electrophysiology
CMROI
- ATP tightly regulated
- glucose consumption
- oxygen consumption
FDG PET
H215O PET
hemodynamic response
- blood flow
- blood volume
- blood oxygenation
fNIR
EEG
fMRI
MEG
Perfusion MRI
Slide 3
Vascular Sensitivity of
fMRI and fNIR
Arterial
Venous
II
Intravascular
fNIR
I
Perfusion MRI
II
fMRI
III
IV
I
Extravascular
III
IV
Vessel Size
CMROI
Slide 4
Vascular Response
fMRI vs fNIR
fMRI
Spatial Resolution
8-27 mm3
Temporal Resolution
Slow (1-2 sec)
Measurement parameter
CMROI
Mix of blood volume, blood
flow, and O2 metabolism
fNIR
“Blobs”
1-10 cm3
Fast (50 Hz)
important?
[Hb] and [HbO]
Slide 5
Mechanisms of fNIR:
Overview

fNIR = functional Near InfraRed


Measure changes in infrared light absorption and scattering
Primary source of signal contrast  [Hb] and [Hb0]

Biological tissue is highly scattering in NIR window

Primarily used in vivo as a spectroscopic modality
 Not used to produce true images

DOT = Diffuse Optical Tomography
 Methods for accurate image reconstruction
CMROI
Slide 6
Mechanisms of fNIR:
Absortion of [Hb] and [Hb0]
Water Absorption
• Near infrared “window” ~ 650-900 nm
• Water absorption is mimized
• Hemoglobin species are dominant absorbers
[Hb] & [HbO] Absorption
CMROI
Slide 7
Mechanisms of fNIR:
Beer-Lambert Law
Beer-Lambert law models ballistic photon propagation in absorbing media
Transmittance, T = I/Io
Absorbance, A = -log(I/Io)
Beer-Lambert Law:
A =  [X] d
d
Io
where:
d = distance between I0 and I
 = absorptivity (M-1 cm-1)
[X] = concentration of absorber (M)
I
solution
CMROI
[X]
Slide 8
Mechanisms of fNIR:
Modified Beer-Lambert Law
Photons travelling through biological
tissue are highly scattered (not
ballistic)
Scattering adds to “pathlength”
travelled by photons
Source
Detector
Detector
d
shallow
deeper
Modified Beer-Lambert Law:
(
Fat
Muscle
Source-detector spacing influences depth penetration
A = -log(I/Io) =  [X] d  DPF + G
where:
DPF = differential pathlength factor
G = Scattering loss factor (generally unknown)
CMROI
Slide 9
Mechanisms of fNIR:
Measures Changes in [Absorber]
• Scattering factor, G, is unknown
• Absolute concentrations are not derivable
• Can measure changes in [Hb] & [HbO]
• Need baseline assumption or independent measure of [Hb]
Measure [Absorber]
A2–A1 = -log(I2/I1) =  [X] d  DPF
where:
A2,A1 = absorption measured at two time points
CMROI
Slide 10
fNIR Methodology: Tissue
Penetration
• NIR light penetration into biological tissue allows for surface imaging
• Penetration increases with source light intensity
• Limits on safe levels of source light intensity (~1mW/mm2)
• SNR  sqrt(Io)
• Highly sensitive detectors (PMTs) allow 2-6 cm deep probing
CMROI
Slide 11
fNIR Methodology:
Quantitation of Multiple Chromophores
Multiple absorbers ([Hb], [Hb0])  multiple wavelengths
Extension of MBLL to multiple absorbers:
(MBLL):
A1 = (Hb 1[Hb] + HbO1[HbO])  d  DPF
A2 = (Hb 2[Hb] + HbO2[HbO])  d  DPF
1 2 3
Source illumination is time or frequency
multiplexed at several wavelengths.
CMROI
Slide 12
fNIR Methodology:
Temporal Resolution
Extremely high temporal resolution possible
Practical systems ~ 10 – 100 Hz
fMRI ~ 1-2 Hz
Hemodynamic changes are slow ~ 2-5 sec
Fiber-optic systems for simultaneous fMRI
Fast signal – cell conformation and swelling
Scattering changes > 10 Hz
Extremely low signal
Ellusive to date
from Strangeman Biol Psych 2002
CMROI
Slide 13
fNIR Methodology:
Spatial Localization
Discrete arrays of sources and detectors
# voxels = # sources  # detectors
Typical systems  10 – 100 voxels
Poorly localized “blobograms”
Resolution  1-8 cm3
Surface FOV
Compare to low-res fMRI: 64x64x30  217 voxels!
Whole brain coverage
CMROI
from Franceshini, NeuroImage, 2004
Slide 14
fNIR Methodology:
Spatial Localization with DOT
True tomographic methods ~ 10,000 S-D pairs
Flying spot illumation
(r)
CCD detection
Low temporal resolution ~10 – 100 sec / image
ill suited for functional assessment
“Hitting Density”,  – poor basis set
undetermined inversion problem
A = (r) (r) dr
 = Hb[Hb] + HbO[HbO])
CMROI
from Strangeman Biol Psych 2002
Slide 15
fNIR Methodology:
MBLL vs DOT
CMROI

Many fNIR implementations report [Hb]
changes from individual S-D pairs w/o
attempt at DOT

DPF in MBLL calculated from uniform
background absorption and scattering.
Focal changes not properly modelled.

“MBLL and DOT results did not agree in
terms of absolute magnitudes, relative
magnitudes, or even the relative sign for
changes in [HbO] and [Hb].” (Boas,
NeuroImage, 2001)
Slide 16
Spatial Maps of HRF Metrics:
TTP Maps
CMROI
Slide 17
fMRI: Mental Chronometry
ADC compartmentalization resolves events separated by 125ms.
TTP Map
1 second right fovea & auditory delay
CMROI
Slide 18