Shengwen Deng1, Eric Muir2, Wei Zhou3, and Timothy Q. Duong2
1University of Texas Health Science Center at San Antonio, San Antonio, TX, United States, 2University of Texas Health Science Center at San Antonio, 3Radiology, Mayo Clinic
Synopsis
T1 mapping is showing great
potential for mapping oxygen in human organs such as eyes and lungs. And yet,
accuracy of oxygen using fast T1 imaging methods is of great concern especially
in tissue with radical temperature changes. In the current study we improve fast
T1 mapping with temperature correction and explore its potential in mapping
oxygen in eyes. With combination of inversion-recovery Look-Locker bSSFP and diffusion weighted thermometry, we calibrate the temperature dependence of ADC and T1, and use
it to adjust the R1 for measuring partial pressure of oxygen(pO2). Fast T1
mapping could be a reliable way to pO2 that well agrees with invasive oxygen-sensitive
optic fibers.
PURPOSE: Fast T1
mapping has been used to noninvasively measure partial
pressure of oxygen in human vitreous due to the paramagnetic oxygen molecule. Previous studies found the
accuracy of PO2 mapping is sensitive to temperature gradient across the eye
between close and open condition.[1] The aim of this study is to calibrate T1 measurement
with
temperature correction and apply it to mapping oxygen in ex vivo eye, which is
99% water. Calibration of T1 and Apparent Diffusion Coefficient (ADC) at
different PO2 and temperature were performed on water phantoms and ex vivo eyes.
The temperature will be estimated via ADC-based thermometry in the phantoms,
and used to adjust the T1 variation in different temperature. Non-invasive PO2
measurement with temperature correction from MRI were then compared with the
exact PO2 concertation measured by oxygen-sensitive fiber optic probe.
METHODS: Phantoms filled with distilled water were bubbled with
nitrogen to different pO2 concentrations (n=7 for calibration and 4 for validation).
pO2 was confirmed by oxygen optode (Oxylab, Oxford Optronics). Enucleated canine
eyes (n=2) were kept in saline and studied within 12 hours of necropsy. After
MRI, the pO2 probe was inserted into the vitreous and the phantoms to measure pO2.
Samples were immersed in circulating water to control temperature from 23-40.2oC,
monitored by temperature probe. MRI was performed at 3T with receive-only head coil. T1 measurements were made using inversion-recovery
Look-Locker balanced steady-state free-precession (bssfp) with TE/TR=2.3/5.3ms, 21 TI from 340-10,000ms, FOV=100x100mm, matrix=176x176, 5mm slice, sequential sampling and FA=35o (and 70o for flip angle
correction). Single shot Diffusion weighted EPI was used with b-value=0 and 100, TE/TR=78/6000ms. T1 and ADC were
fit pixel-by-pixel. Linear
regression was used to determine the slope and intercept of R1 vs pO2, ln(ADC) vs
1/Temp, and –ln(T1) vs 1/Temp (in K).[1,2]1[em1] Interclass cross correlation was used to find the agreement of estimated
pO2 after temperature correction as a function of pO2 measured by invasive
optode.
RESULTS: With water phantoms (n=7), the relationship between R1 with pO2 at 37oC
were found to be R1= [pO2]*2.00x10-4s-1/mmHg+0.2187s-1.T1
as a function of temperature with different pO2 concertation has a slope of 1.883+_ 0.08474, the R1
value of vitious is slightly higher than that of water with similar pO2. ADC as a function of temperature had slope of 8E-05/oC,
with value from 0.0015 to 0.0039. ADC in different direction has different
measurement error (standard error from 0.22(x-direction) to 1.68(z direction)
at 36.8 oC). Using another set of phantom for validation (n=4), we
found that the relation of R1 with pO2 can be merged together and giving the
equation of R1= [pO2]*2.73x10-4s-1/mmHg+0.2149s-1. Ex vivo vitreous (pO2 of 8.9
and 3 mmHg from optode) had with R1 of 0.2258s-1 and 0.2235s-1
respectively at 37o, which is offset from water at 37oC and same pO2
by s-1 . Using previously measured vitreous offset of s-1
the ex vivo vitreous would have pO2 from bSSFP would be 5 mmHg and -4 mmHg[1]. Interclass cross correlation of estimated PO2
and PO2 measured after the scan is 0.9901, with a f value of 0.64 indicating
good agreement between the different measurement of oxygen.
DISCUSSION:
The sensitivity to temperature
has been considered as great impact factor in mapping oxygen in eyes. Some
groups has shown that T1 could be adjusted via the linear relationship at the
temperature around 35°C.[4]
Our data, for the first time, quantify the temperature dependence of T1 value
in fast T1 mapping methods and illustrate adjusting method that will work in physiological
temperature (24 to 40°C).
With this technique, the pO2 measurement
in MRI can be as robust as the invasive oxygen-sensitive optic fibers in pure
water and virtuous. Previously report data indicated that ADC has
temperature sensitivity around 1.94-2.49%/°C[5], which agree well with our
speculation. Even so, the noise and artifact in ADC maps is considered as the he
major source affecting the accuracy of temperature correction. Though there has been concern that fast look-locker bSSFP
mapping may underestimated the T1 value compared to inversion-recovery FLASH, our
data suggests that this sequence is robust in mapping oxygen with varying range
of temperature. This may provide options
for imaging oxygen in eye with greater accuracy in an acceptable time.
In conclusion,
temperature corrected fast T1 MRI could be used to non-invasively map
oxygenation of the vitreous with considerable accuracy. Future studies will
improve off resonance effect in T1 mapping of in vivo eye, exploring b- value correction
and eliminate the ghosting artifacts in EPI for imaging the in vivo virtuous.
[em1]Hindman et alAcknowledgements
Eric
Muir, Ph.D holds a Voelcker Fund Young Investigator Award from the Max and
Minnie Tomerlin Voelcker Fund.References
Reference:
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pressure[J]. Radiology, 2013, 266(3): 905-911.
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Wood M. Relaxation processes in water. A study of the proton spin-lattice
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"Measuring the Effect of Pars Plana Vitrectomy on Vitreous Oxygenation
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Investigative ophthalmology & visual science 54.3 (2013): 2028-2034.
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"A feasibility study on monitoring the evolution of apparent diffusion
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