Enhancement of signal intensity using a wireless coil for FT-EPR oximetry study
Ayano Enomoto1, Gadisetti V. R. Chandramouli2, Alan P Koretsky3, Chunqi Qian4, Murali K Cherukuri1, and Nallathamby Devasahayam1

1Radiation Biology Branch, National Cancer Institute, Bethesda, MD, United States, 2GenEpria Consulting Inc., Columbia, MD, United States, 3National Institute of Neurological Disorders and Stroke, National Institutes of Health, Bethesda, MD, United States, 4Department of Radiology, Michigan State university, East Lansing, MI, United States

Synopsis

Sensitivity enhancement is required to detect the weak signals with Fourier transform Electron Paramagnetic Resonance (FT-EPR). In the proposed method, a small amount of sample was placed at a distance less than half the diameter of the receiving surface coil. The signal was enhanced by a wirelessly pumped coil. Presently, we used the TCNQ for our studies to study signal enhancement. Here, we achieved 7-fold of improvement in signal intensity in compared with conventional FT-EPR acquisition. We will show the results of in vivo oximetry using oxygen sensing solids LiPc and LiNc in in vivo applications to measure tissue oxygenation.

Purpose

The purpose of this study is to investigate the feasibility of signal enhancement using the wireless coil in Fourier transform electron paramagnetic resonance (FT-EPR) system for high sensitive repeated oximetry measurements. The knowledge of temporal change in partial pressure of oxygen (pO2) in tissue is important for understanding the pathology of hypoxia related diseases. The EPR oximetry is the one of the strong methods for repeated monitoring pO2 over time1,2. For repeated EPR oximetry, the signal from the reagents implanted in such as lithium phthalocyanine (LiPc) or lithium naphthalocyanine (LiNC)3 is so weak in the presence of oxygen that it is difficult to detect with 300 MHz FT-EPR. Therefore, improvements in sensitivity of detection is required to achieve high sensitive oximetry in 300 MHz FT-EPR. In magnetic resonance imaging (MRI), there are some reports to detect and enhance signals from deep lying internal organs by using a wireless coil which enables weak signal to amplify4,5. We applied the same principle using the wireless coil to 300 MHz FT-EPR and attempted to increase the detection sensitivity of FT-EPR.

Methods

A wireless coil is a detector using parametric amplification, which can amplify the weak signal by applying some power (pumping power) through the inductive coupling with external coil (pumping coil). The detailed theory and construction of the wireless coil has been reported earlier5. To evaluate the effect of using wireless coil, we obtained spectra using a homebuilt 300 MHz FT-EPR for the all measurements in this study. The parameters of measurements were as follows: repetition time, 10 µs; 90 degree pulse width, 80 ns; number of average, 100000 times; transmit power, 64 W. The surface coil resonator with 22 mm diameter coil was used as transmitter and receiver. The quality factor of the resonator was set to around 30 to reduce dead time. The resonant frequency of the wireless coil was set to 300 MHz for idler signal and amplified signal, and 600 MHz for pumping signal. The diameter of the pumping coil for pumping the wireless coil was also 22 mm. The sample was a cylinder (2 mm inner diameter and 1.5 mm height) filled with solid N-methyl pyridinium tetra-cyanoquinodimethane (TCNQ). Figure 1 shows the configuration of the measurements and the pictures of the coils.The EPR measurements were repeated under different conditions: a) without the wireless coil (normal EPR measurement); b) with wireless coil and no pumping power; and c) with wireless coil and pumping power.

To determine the peak pumping power accurately, we performed experiments under the slightly different magnetic field from original zero magnetic field (10.7 mT). That enabled us to distinguish the signal generated by electron spin from the signal due to the oscillation signal of wireless coil. The pumping power at which we got the highest peak related to 300 MHz was the peaking power. Then the pumping power was reduced step by step until the zero frequency disappeared. It was found at that time the enhancement of signal due to pumping frequency was high. Then the magnetic field was changed to zero magnetic field and the measurements were made.

Results and Discussion

Figure 2 shows the results of the FT-EPR spectra with and without the wireless coil. Without the wireless coil and with the wireless coil but no pumping power, the signal intensity was 0.53 and 0.49, respectively. When the proper pumping power (in this case 1.46 dBm) was applied to the wireless coil, the signal intensity was increased to 3.82. The line width got narrow when the wireless coil was placed. However, since the calibration curve will be constructed before EPR oximetry, the change of line width does not affect to measurements of oximetry. Figure 3 shows the relation between the signal level and applied pumping power. When the pumping power was decreased, the signal intensity was also decreased. When pumping power was more than the proper pumping power (1.46 dBm), the signal from the electron spin was hidden by the oscillation signal generated by the wireless coil itself.

Conclusion

We have demonstrated the feasibility of enhancement of sensitivity by using the wireless coil to FT-EPR. We succeeded to increase the signal intensity 7 times compared with conventional FT-EPR measurement. This shows it is possible to detect the small signal with FT-EPR using wireless coil. Therefore we will apply the wireless coil to in vivo oximetry in future applications.

Acknowledgements

No acknowledgement found.

References

1. Matsumoto S, Espey MG, Utsumi H, Devasahayam N, Matsumoto K, Matsumoto A, Hirata H, Wink DA, Kuppusamy P, Subramanian S, Mitchell JB, Krishna MC. Dynamic Monitoring of Localized Tumor OxygenationChanges Using RF Pulsed Electron ParamagneticResonance in Conscious Mice, Magn Reson Med. 2008; 59(3): 619-625.

2. Swartz HM, Khan N, Buckey J, Comi R, Gould L, Grinberg O, HartfordA, Hopf H, Hou H, Hug E, Iwasaki A, Lesniewski P, Salikhov I, WalczakT. Clinical applications of EPR: overview and perspectives. NMR Biomed. 2004 Aug; 17(5): 335-351.

3. Ahmad R, Kuppusamy P. Theory, Instrumentation, and Applications of EPR Oximetry. Chem Rev. 2010; 110(5): 3212-3236.

4. Qian C, Murphy-Boesch J, Dodd S, Koretsky A, Sensitivity enhancement of remotely coupled NMR detectors using wirelessly powered parametric amplification. Magn Reson Med. 2012; 68(3): 989–996.

5. Qian C, Yu X, Chen DY, Dodd S, Bouraoud N, Pothayee N, Chen Y, Beeman S, Bennett K, Murphy-Boesch J, Koretsky A. Wireless Amplified Nuclear MR Detector (WAND) for High-Spatial-Resolution MR Imaging of Internal Organs: Preclinical Demonstration in a Rodent Model. Radiology. 2013; 268(1): 228–236.

Figures

Figure 1. A: The configuration of measurements. The wireless coil was put on the sample. B: the picture of each coil and sample. The sample was covered with tape.

Figure 2. Comparison of the signal intensity between when conventional measurement was performed and when proper pumping power was applied to wireless coil. These spectra were obtained at zero field (11.7 mT).

Figure 3. The change of the signal intensity giving different power less than proper pumping power.



Proc. Intl. Soc. Mag. Reson. Med. 24 (2016)
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