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Fast T1rho mapping in mice using an optimized Bloch simulation based radial sampling pattern
Maximilian Gram1,2, Daniel Gensler1,3, Patrick Winter1,2, Michael Seethaler2,3, Peter Nordbeck1,3, and Peter Jakob2
1Department of Internal Medicine I, University Hospital Würzburg, Würzburg, Germany, 2Experimental Physics 5, University of Würzburg, Würzburg, Germany, 3Comprehensive Heart Failure Center (CHFC), University Hospital Würzburg, Würzburg, Germany

Synopsis

Myocardial T-mapping in small animal studies is still a challenging procedure. Commonly, T-mapping requires long measurement times or only provides insufficient image quality due to a low signal-to-noise-ratio. Using a novel approach based on an optimized radial sampling pattern and high flip angles, we were able to overcome both restrictions. By a special sorting of golden angles based on Bloch simulations the image quality of the method could be significantly increased, and a high quantification accuracy could be realized. Thus, the new approach is a reliable method for fast T-mapping in future studies on small animals.

Introduction

In the field of cardiac MRI, numerous studies have pointed to the alternative contrast mechanism of the spin-lattice relaxation time T under the spin-lock (SL) condition [1,2,3]. It has been shown that T provides a high endogenous contrast between healthy myocytes and collagenous scars in cardiac tissue [1]. For this, myocardial T-mapping is of great interest for improved imaging and diagnostics of cardiac diseases in animal models. Due to the high heart rate and the special concept of SL preparation, acquisition of T-maps in small animals is quite challenging. Hence, commonly used T-mapping sequences require long measurement times or only provide an insufficient image quality due to a low signal-to-noise-ratio.Therefore, it is crucial to establish new methods to overcome both restrictions generating accurate and high-resolution T-maps within very short scan times. In this work, we present a new highly accelerated and optimized approach for myocardial T-mapping that allows the acquisition of a T-map in less than two minutes.

Methods

All measurements were performed on a 7.0T small animal imaging system (Bruker BioSpec 70/30, BioSpin MRI GmbH, Ettlingen, Germany). Acquisition of k-space was optimized for very fast myocardial imaging using a radial spoiled gradient echo readout (TE=1.9ms, TR=4.7ms). T preparation was performed by totally-balanced-spin-locking (TB-SL) [4]. A key point of the new concept was to increase the SNR by using high flip angles (α=45°) in the readout. Due to the resulting high signal changes during data acquisition, an optimized sampling scheme is required. For every T-weighted image, data sampling was segmented into 13 preparation experiments (with identical preparation times tSL), acquiring four radial spokes after the SL preparation (Fig. 1). In order to generate T-maps, a series of 8 T-weighted images with different tSL is acquired, leading to 13x8=104 consecutive preparation experiments in total. The acquisition window was positioned in end diastole using a suitable trigger delay (depending on tSL). Each preparation experiment was separated by a waiting time trec for magnetization recovery, which is dependent on the respiratory cycle rate resulting in a total measurement time of approximately 2min.

For k-space sampling, three different golden angle sorting schemes were used and compared (Fig. 2). First a serial sampling, at which subsequent golden angles were increased in every subsequent TR. Second an echo number based sampling, at which subsequent golden angles were assigned to the acquisition number after the preparation module. And finally, our novel Bloch simulation based sampling, at which subsequent golden angles were assigned to the expected signal intensity of the corresponding acquisition window. For this, the signal intensity for every acquisition window is simulated using the known sequence timings and estimated T1 and T values of the probe under investigation. For all three sampling schemes, image reconstruction was performed using a KWIC filtered view sharing method [5]. Here, the k-space center for a desired T-weighting (with desired tSL) is exclusively selected from the first acquisition window after preparation. The k-space peripherals were also chosen from other acquisition windows as well as other T-weightings.The three sampling schemes were compared in phantom measurements consisting of four cylindrical sample tubes with different concentrations of BSA (Bovine Serum Albumin) analyzing the SNR and artifact susceptibility of the methods. Furthermore, myocardial T-mapping with our Bloch simulation based sampling scheme was performed on mice. The achievable image quality was compared with the echo based sampling using low flip angles (10°).

Results

Fig. 3 shows the results of the SNR and artifact analysis. Our optimized Bloch simulation sorting of the golden angles causes a significant increase in SNR by a factor of 3.09 compared to the serial sorting and by a factor of 1.34 in relation to the echo position sorting. Analysis of the T quantification accuracy revealed a maximum deviation of smaller than 1.7% in comparison to a cartesian fully sampled reference scan (Tab. 1) using our optimized Bloch simulation sampling. The results of the in vivo study show that the use of low flip angles does not provide sufficient SNR for myocardial T-mapping. In contrast, our new method based on high flip angles and Bloch sorting provides a significantly higher image quality. Compared to the cartesian reference scan, the measurement time was reduced by a factor of 1.8 to less than 2 minutes (depending on the respiratory cycle).

Discussion

In the presented work, we introduced a novel fast myocardial T-mapping sequence using an optimized sampling scheme and high flip angles. The phantom and in vivo measurements showed that our new method provides a high SNR and excellent image quality. Using significantly undersampled radial data, a very short measurement time of less than 2 minutes could be achieved. In addition, the use of a radial data acquisition results in a higher robustness against motion artifacts. Due to the very short measurement time, our method enables further detailed T quantification and even T dispersion measurements in vivo during a practicable small animal study protocol. In future measurements, the quantification of T in the myocardium of mice will be studied in detail in specific heart diseases. An ongoing study is focused on myocardial ischemia associated with Fabry disease.

Acknowledgements

This work was supported by the Federal Ministry for Education and Research of the Federal Republic of Germany (BMBF 01EO1504, MO6).

References

[1] Witschey et al. Magn Reson Med. 2010 Nov;64(5):1453-60

[2] van Oorschot et al. J Magn Reson Imaging. 2015 May;41(5):1181-9

[3] Kamesh Iyer et al. J Cardiovasc Magn Reson. 2019 Jan 10;21(1):5

[4] Gram et al. ISMRM Annual Meeting 2019. Montreal. #1215

[5] Song et al. Magn Reson Med. 2000 Dec;44(6):825-32.

Figures

Fig. 1) Sequence sampling scheme for myocardial T-mapping. After prospective respiratory gating, a trigger on the R-wave is used followed by an appropriate trigger delay and the SL preparation (TB-SL [4]). Thereafter, 4 radial spokes of k-space are acquired in end-diastole during one heartbeat. This procedure is repeated in each respiratory cycle. For each T-weighting, 13 (Fibonacci number) repetitions are used.

Fig. 2) Simulated and measured signal intensity for various SL preparations illustrating the different sampling schemes. The numbers represent the indices of the acquired golden angles. The colors of the plateaus represent the different acquisition windows after SL preparation (cf. Fig. 1). For echo number sorting, the golden angles were ordered by the acquisition number after preparation. With Bloch simulation based sorting, the golden angles were ordered by the expected signal intensity.

Fig. 3) Comparison of the different sampling schemes using reconstructed T-weighted images of four BSA phantoms. In the upper row, the images are “normally” scaled. In the bottom row, the scaling is adapted to highlight artifacts. It is apparent that the Bloch sorting produces the least artifacts. The SNR is increased by a factor of 3.09 and 1.34. For Bloch simulation the known sequence parameters and the estimated relaxation times T1=1400ms and T=40ms were used.

Tab. 1) Comparison of T quantification between the accelerated KWIC filter method (Bloch sorting) and a cartesian reference measurement. The results of four BSA phantoms with different concentrations were evaluated using three different SL amplitudes fSL. The SL time was varied in the range 4-128ms. The maximum deviation observed was 1.61%.

Fig. 4) Comparison of low (10°) and high (45°) flip angles in the in vivo experiment of mice (short axis view, isotropic resolution 260µm). The T weighted images were reconstructed using our new accelerated method. The T-maps were calculated by pixel-wise fitting a mono-exponential function. The SL times were varied in the range of 4-64ms. The SL amplitude was 1500Hz. Due to the high flip angle of 45°, the Bloch sorting sampling with assumed values of T1=1200ms and T=40ms was used.

Proc. Intl. Soc. Mag. Reson. Med. 28 (2020)
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