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Fixed-Point MR Imaging for Early Gliobrastoma Detection
Zhao Li1, Chao-Hsiung Hsu2, Huiyuan Zheng2, and Yung-Ya Lin2

1Chemistry and Biochemistry, UCLA, Los Angeles, CA, United States, 2UCLA, Los Angeles, CA, United States

Synopsis

Problem Early detection of high-grade malignancy, such as GBM, remains challenging using MRI.

Methods A new approach using continuous-wave and feedback field to reach “fixed-point spin dynamics” was developed to enhances the local magnetic-field gradient variations due to irregular water contents and deoxyhemoglobin concentration in early GBM.

Results In vivo MR images and mappings acquired on orthotopic GBM mice using “fixed-point pulse sequence” shows 3-4 times of enhancement in GBM contrast than the best conventional images acquired.

Conclusion Simulations and in vivo GBM mouse models validated the superior contrast/sensitivity and robustness of fixed-point spin dynamics method towards early GBM detection.

Introduction

Early detection of high-grade malignancy, such as glioblastoma multiforme (GBM), using enhanced MRI techniques significantly increases not only the treatment options available, but also the patients’ survival rate. For this purpose, a conceptually new approach, named “fixed-point MR imaging”, was developed. An active feedback electronic device was homebuilt to implement active-feedback pulse sequences to generate avalanching spin amplification and fixed-point spin dynamics, which enhances the local magnetic-field gradient variations due to irregular water contents and deoxyhemoglobin concentration in early GBM.

Methods

The general principles of the “active-feedback controlled MR” and details in the device design can be found in our publications. 1-5 Here, the specific pulse sequence to carry out the “fixed-point MR imaging” and its applications to early GBM detection were developed and demonstrated.

(i) First, an active-feedback electronic device was home-built to generate feedback fields from the received FID current. The device is to filter, phase shift, and amplify the signal from the receiver coils and then retransmit the modified signal into the RF transmission coil, with adjustable and programmable feedback phases and gains, allowing us to utilize the active feedback fields in novel ways.

(ii) Next, an innovative pulse sequence was developed for early GBM detection and was statistically tested on in vivo orthotopic GBM mice models, as shown in Fig. 1. It is a phase-cycled repeating block of [cw-pi-cw], where active-feedback field is also on during the cw (continuous wave) pulse to enhance the contrast originated from local magnetic-field gradient variations due to irregular water contents and deoxyhemoglobin concentration in early GBM. In essence, the enhanced GBM contrast arises from “selective self-excitation” 6 and “fixed-point dynamics” (discussed below) generated by the bulk water 1H under active feedback fields.

(iii) Computer simulations for a simple two-component system with small resonance offset and a more realistic early GBM model based on blood-oxygen-level-dependent (BOLD) model 7,8 were carried out (Fig. 2 and Fig. 3, respectively).

(iv) In vivo images of orthotopic GBM mouse models were acquired on a 300 MHz microimaging system incorporated with our active-feedback device (Fig. 4 and Fig. 5).

Results

Stage-1 orthotopic GBM mouse models infected with human U87MG cell line were imaged. Representative results from 2 mice were shown in Fig. 4 and Fig. 5. For a very early stage GBM model (4 days after tumor implantation), fixed-point image shows a positive contrast and reaches a maximum contrast of 72.9% between GBM and normal brain tissue, much higher than conventional spin-echo image (-7.3%) and gradient-echo image (4.8%). The early-stage GBM is also highlighted in the time constant mapping of fixed-point images acquired at different preparation time. Since we can freely adjust the strength and phase of our active feedback field using our home-made device, the fixed-point pulse sequence was further improved by incorporating local-field-dependent active feedback phase. Such improved pulse sequence shows a superior contrast than CPMG pulse sequence with very short pi pulse spacing (τCP = 1 ms): 47.7% over 14.7%, as shown in Fig. 5. Statistical results (N=15) show that this new approach provides 3-4 times of improvements in GBM contrast than the best conventional images acquired, as measured by “contrast-to-noise ratio” (CNR) or “percentage contrast” between tumor and normal brain tissue.

Discussion

In dynamical analysis, fixed points are locations in phase space where the evolution of a system is said to cease, without any additional external forces (Fig. 2). Understanding the instability of initial conditions has been used to develop non-linear evolution schemes which can be used to amplify small differences in resonance offset,1 such as is the case between white and gray matter in the brain.4,5 The joint interaction between the continuous wave and the feedback field allows for extended non-linear evolution, capable of producing useful contrast enhancement for imaging purposes. For early stages of GBM growth, differences in magnetic susceptibility originate from variations in blood oxygenation level, increased water content in the compact extracellular space of the tumor, and enhanced angiogenesis (the rapid development of new blood vessels).7,8 The use of a continuous wave in the presence of the active feedback field is able to produce unique fixed-point spin dynamics, resulting in positive, robust contrast between the early-stage GBM and the normal brain tissue.

Conclusion

Computer simulations and in vivo orthotopic xenografts GBM mouse models validated the superior contrast/sensitivity and robustness of fixed-point spin dynamics method towards early GBM detection. Statistical results (N=15) for GBM mouse models at various cancer stages, alternative fixed-point pulse sequences with further improved performance will also be presented.

Acknowledgements

No acknowledgement found.

References

1. Lin YY, Lisitza N, Ahn S, et al. Resurrection of Crushed Magnetization and Chaotic Dynamics in Solution NMR Spectroscopy. Science. 2000;290:118-121.

2. Huang SY, Wolahan SM, Mathern GW, et al. Improving MRI Differentiation of Gray and White Matter in Epileptogenic Lesions Based on Nonlinear Feedback. Magn Reson Med. 2006;56:776-786.

3. Huang SY, Yang SS, Lin YY. Sensitivity of feedback-enhanced MRI contrast to macroscopic and microscopic field variations. Magn Reson Med. 2009;61:925-936.

4. Datta S, Huang SY, Lin YY. Contrast Enhancement by Feedback Fields in Magnetic Resonance Imaging. J Phys Chem B. 2006;110:22071-22078.

5. Huang SY, Furuyama JK, Lin YY. Designing feedback based contrast enhancement for in vivo imaging. Magn Reson Mater Phy. 2006;19:333-346.

6. Li Z, Hsu CH, Dimitrov N, et al. Sensitive Imaging of Magnetic Nanoparticles for Cancer Detection by Active Feedback Magnetic Resonance. Magn Reson Med. 2015;251:33-41.

7. Zimmerman RA, GibbyWA, Carmody R. Neuroimaging: clinical and physical principles. Springer. 2000.

8. Wang G, Tsai SL, Li Z, et al. Towards Early Glioblastoma Detection: In Vivo MR Imaging and Spin Dynamics Simulations (invited paper to Cancers, submitted).

Figures

A fixed-point pulse sequence was developed for early GBM detection and was statistically tested on in vivo orthotopic GBM mouse models. In the preparation part, continuous wave (cw) and feedback (FB) pulses were adapted to generate contrast between early-stage GBM and normal brain tissue.

(A) 3-D trajectory for a two-component system undergoing the fixed-point dynamics, with continuous wave (cw) field strength B1 = 45 Hz and feedback field strength τr = 3.5 ms. The resonance offset of the two components differs by 10 Hz. (B) Time evolution of Mx (x-component of magnetization) for the system described in (A).

For an early-stage GBM modeled by the BOLD model, spin dynamics and simulated contrast by conventional method (spin-echo) and our method (fixed-point) were carried out. (A) Time evolution of Mxy in the spin-echo pulse sequence. The maximum normalized contrast between tumor and brain tissue is 0.053, and the magnetizations die out very fast (within 0.16 s). (B) Time evolution of Mxz in a fixed-point pulse sequence. The maximum normalized contrast is 0.158, and the magnetizations last longer than 0.3 s, leaving a longer acquisition window. (C) When incorporating the local-field-dependent phase (LFDP), the contrast further develops to 0.234.

Representative results from a GBM mouse model acquired 4 days after U87MG cell implantation. Fitted time constants for GBM (in red) and normal brain tissue (in black), and the contrast between them (percentage, in red) were given in the parameter mappings (A and C). Contrast-to-noise ratio (CNR) and percentage contrast between GBM and normal brain tissue were given in the images (B, D, and E). Our active-feedback fixed-point images (B) and decay constant mapping (A) highlight the very early stage GBM with a positive contrast, compared to spin-echo T2 constant mapping (C), spin-echo T2-weighted image (D), and Gradient-echo image (E).

Representative results from a GBM mouse model acquired 17 days after U87MG cell implantation. Fitted time constants for GBM (in red) and normal brain tissue (in black), and the contrast between them (percentage, in red) were given in the parameter mappings (A and C). Contrast-to-noise ratio (CNR) and percentage contrast between GBM and normal brain tissue were given in the images (B and D). Our active-feedback fixed-point images (B) and decay constant mapping (A) show superior contrast to the CPMG image (D) and mapping (C) with very fast pi pulses (τCP = 1 ms) and high SAR.

Proc. Intl. Soc. Mag. Reson. Med. 27 (2019)
4685