Synopsis
It
is extremely challenging to non-invasively measure tissue ROS due to its low
concentration and short lifetime. This study aims to demonstrate a fully
non-invasive CEST MRI method to measure ROS concentration. CEST Z-spectra were
acquired from egg white samples with and without hydrogen peroxide treatment.
In addition, proton exchange rate, T1, and T2 relaxation time
maps were acquired for further clarification on CEST contrast origin. We have demonstrated
that ROS is paramagnetic and can greatly enhance proton exchange rate leading
to reduced CEST contrast.Target audience
Scientists
or clinicians interested in oxidative stress, reactive
oxygen species, and
CEST MRI.
Purpose
Oxidative stress due to elevated reactive oxygen species
(ROS) is a critical contributor in various processes including normal aging,
Alzheimer's disease, stroke, cardiac arrest, cancer, and diabetes (1-3). Direct and non-invasive approaches for quantifying tissue ROS will provide useful information in early diagnosis,
disease stratification, and treatment response. Given that ROS has an extremely
short lifetime (~10
-9 s for hydroxyl radicals) (4), and its
in-vivo concentration is in µM level(5), it has been
difficult to perform direct measurement. Currently there is no direct and
non-invasive method to assess ROS production (6-9). In this study, we aim at developing a
fully non-invasive method to measure tissue ROS concentration based on endogenous
MRI contrasts including the chemical exchange saturation transfer (CEST)
contrast that origins from exchangeable protons associated with specific metabolites.
Methods
We investigated CEST MRI properties of ROS produced by
adding hydrogen peroxide (H
2O
2)
into
ex-vivo tissues. Fresh egg
white tissues (n=5) treated with various concentrations of H
2O
2
(0.25, 0.1, 0.05, and 0.025 v/v%) were scanned at different time points(0.5, 1,
and 3 hours) at room temperature. Fluorescence studies using the hydroxyphenyl fluorescein (HPF) dye were
performed to measure ROS production from the samples treated within 1 hour. CEST
Z-spectra were collected on a horizontal 9.4-T MRI scanner using a customized
sequence with a frequency-selective rectangle saturation pulse (B
1=50
Hz, 3 s) followed by a Fast Low-Angle Shot (FLASH)
readout. The entire Z-spectra contained 49 saturation offsets ranging
from -5 to 5 ppm with steps of 0.25 ppm, and at ±10, ±20, ±50, and ±100 ppm. CEST asymmetry effect was computed at 3.5
ppm. In a separate study, the proton exchange rates of untreated and treated
(0.1 v/v% H
2O
2) egg white samples (n=4) were assessed based
on the method previously described (10). The steady-state CEST images
were acquired with a 4 s long saturation pulse at various saturation amplitudes
B
1 from 50 up to 450 Hz. Data were fitted with a polynomial function
to determine the amplitude leading to the maximal steady-state CEST contrast.
In addition, T
1, T
2, and pH were measured.
Results and
Discussion
Compared to untreated egg white samples, H
2O
2
treatment modulated the entire CEST Z-spectra (Figure 1A), resulting in reductions
in the CEST contrast. The CEST contrast reduction was proportional to H
2O
2
concentration (Figure 1B). Fluorescence studies showed that ROS
production was also proportional to H
2O
2 treatment
concentrations (Figure 1C). Interestingly, the required saturation
amplitude for the maximum
steady-state CEST contrast was much higher for the treated samples than the
untreated, indicating that ROS greatly enhances proton exchange rate (Figure 2). Since
CEST contrast relies on slow-to-intermediate proton exchange, we believe that
ROS reduces CEST contrast by substantially raising the proton exchange rate. In
addition, pH measurements showed only minor changes between baseline and at 1
hour post-treatment with 0.25 v/v% of H2O2 (pH = 9.00 ±
0.01 vs. 8.92 ± 0.01). These suggest that ROS likely serves as an independent
exchange modulator from pH.
We also found that T
1 relaxation time in egg
white reduced due to H
2O
2 treatments, while the reduction
in T
2 relaxation time was negligible (Figure 3). This indicates that
ROS has a strong paramagnetic effect that can be detected by T
1-weighted
MRI. In contrast, intact H
2O
2 (in PBS) does not affect T
1
significantly.
At 3 hours post treatment, CEST contrast recovered almost
back to the pre-treatment level (Figure 4), indicating all the H
2O
2
was converted to ROS within this time. We modeled the dynamics of CEST contrast
as an exponential decay function and estimated that the ROS concentration (with
0.025 v/v% H2O2 at 1 hour post-treatment) was about 50 µM,
which is within the in-vivo pathological
or physiological range (5, 11, 12). We are currently working toward the in-vivo applications of this technique.
Conclusion
In summary, we have observed that ROS is paramagnetic. ROS
also greatly enhances proton exchange, independent to pH, leading to reduced
CEST contrast in general. We have showed that CEST combined with T
1-weighted
contrast has the potential to improve the specificity for imaging ROS or
oxidative stress in tissue. This novel MRI technique may serve as a
longitudinal imaging tool for biochemical analysis of ROS production in ex-vivo tissue or other experimental set-ups.
It may also allow for non-invasively quantifying and mapping ROS production in
vivo with high temporal and spatial resolutions.
Acknowledgements
No acknowledgement found.References
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