Di Guo1, Zhangren Tu1,2, Tianyu Qiu3, Xiaofeng Du1, Min Xiao2, Vladislav Orekhov4, and Xiaobo Qu3
1School of Computer and Information Engineering, Xiamen University of Technology, Xiamen, China, Xiamen, China, 2School of Opto-Electronic and Communication Engineering, Xiamen University of Technology, Xiamen, China, Xiamen, China, 3Department of Electronic Science, Xiamen University, Xiamen, China, Xiamen, China, 4Department of Chemistry and Molecular Biology and Swedish NMR Centre, University of Gothenburg, Gothenburg, Sweden, Gothenburg, Sweden
Synopsis
Accelerating the data acquisition is one of the major developments in modern Nuclear Magnetic Resonance (NMR). Non-Uniform Sampling (NUS) acquires fewer data and reconstructs the spectra with proper signal processing methods1. Here, we introduce an approach to reconstruct faithful spectra from highly accelerated NMR. The FID signal is constrained by the self-learning signal subspace (SLS), in which a true representation of NMR should be in. Results on realistic NMR data demonstrate that the new approach provides much better spectra than the compared state-of-the-art method.
Purpose
Fast Nuclear Magnetic Resonance (NMR) spectroscopy is strongly desired in modern biochemistry applications2, 3, especially for high-dimensional spectroscopy of macromolecule4. The acceleration factor has been gained by fast sampling, however, it is always limited because the compromised spectra quality achieved when applying a high acceleration factor. Although the low-rank Hankel Matrix (LRHM)5-7 can reconstruct broad peaks, low intensity peaks may be submerged when the data is highly undersampled . Since the singular values mainly correspond to the peak intensity, solely manipulating the singular values may ignore the peak shapes, which are of great importance in NMR spectroscopy8. Therefore, the original LRHM method is at the risk of distorting peak intensity and shapes, particularly for the FID with very limit sampled data9. Herein, we propose a self-learning signal subspace (SLS) method to enable reliable reconstruction of the low-intensity peak even when substantial acceleration factor is applied.Method
In NMR, the Free
Induction Decay (FID) signal is usually modeled as the sum of exponential
functions as$$ {x_m} = \sum\limits_{j = 1}^J {\left( {{A_j}{e^{i{\phi _j}}}} \right){e^{ - \frac{{m\Delta t}}{{{\tau _j}}}}}{e^{im\Delta t{\omega _j}}}} ,(1) $$
where $$$ J $$$ is the number of
spectral peaks,$$${A_j},{\phi _j},{\tau _j},{\omega _j}$$$are the amplitude, phase, decay time and frequency of the spectral peak, respectively.
The
LRHM minimizes the nuclear norm, the sum of singular values, as an indicator of
the rank of Hankel matrix. This scheme may result in unsatisfactory
reconstruction because of suppressing or even removing small but meaningful
singular values.
In this work, a self-learning signal subspace (SLS) method
is proposed to enable reliable reconstruction of the low-intensity peak even
when substantial acceleration factor is applied. Let the FID be recovered as $$${\bf{x}}$$$, then the reconstruction problem is formulated as$$ \mathop {{\rm{min}}}\limits_{\bf{x}} {P_r}\left( {\bf{x}} \right) + \frac{\lambda }{2}\left\| {{\bf{y}} - {{\cal U}}{\bf{x}}} \right\|_2^2,(2) $$
where$$${P_r}\left( {\bf{x}} \right) $$$is defined as
$$ {P_r}({\bf{x}}) = {\left\| {{{\cal R}}{\bf{x}}} \right\|_ * } - Tr\left( {{{\bf{A}}_r}{{\cal R}}{\bf{xB}}_r^H} \right), (3)$$
where $$$ {{\bf{A}}_r} $$$ and $$${{\bf{B}}_r}$$$ are two matrices
formed by the first r columns of the left
and right unitary matrixes that satisfy singular value decomposition in $$$ {{\cal R}}{\bf{x}}{\rm{ = }}{\bf{A\Lambda }}{{\bf{B}}^H}$$$ and
which is the subspace of the reconstructed signal, $$${ \bullet ^H} $$$ is complex conjugate
transpose, $$${{\cal R}}$$$ denote an operator converting the FID $$${\bf{x}}$$$ into a Hankel
matrix $$${{\cal R}}{\bf{x}}$$$,$$$ Tr\left( \cdot \right) $$$ is trace function, $$${\left\| \cdot \right\|_*}$$$represents
the nuclear norm, $$$ {\left\| \cdot \right\|_2} $$$ represents
the $$$ {l_2} $$$ norm, $$$ \lambda $$$ denotes a
regularization parameter that balances the two terms, and $$$ {{\cal U}} $$$ is an undersampling operator. In our implementation, $$$ {{\bf{A}}_r} $$$and $$${{\bf{B}}_r}$$$ are first estimated
from the NUS FID and then updated from the reconstructed FID for better
accuracy. Results
The reconstruction performances of
proposed SLS and LRHM are evaluated on realistic biological protein MRS.
The
sample is 2 mM U-15N, 20%-13C GB1 in 25 mM PO4, pH 7.0 with 150 mM NaCl and 5%
D2O. Data was collected using a phase-cycle selected HSQC at 298 K on a
Bruker Avance 600 MHz spectrometer using a room temp HCN TXI probe, equipped
with a z-axis gradient system. Since the singular value mainly correspond to
the peak intensity as shown in Figure 1, The more accurate the peak signal space, the better the reconstruction. Obviously, The SLS
reconstructs the spectral peaks better than the LRHM (Figure. 2(f) and (g)),
particularly for peaks with low intensity (Figure. 2(e)).Conclusion
A self-learning
signal subspace method is proposed to reconstruct the
sparsely sampled data in fast NMR spectroscopy. A major advantage of this model is that weak peak are better preserved
in reconstruction. This method may also
be useful to magnetic spectroscopic imaging (MRSI) in which the weak spectral
peaks may be distorted in data processing.Acknowledgements
This work was supported in part by the National Natural
Science Foundation of China (61871341,
61971361, 61571380, 61811530021, U1632274), the National Key R&D Program of China (2017YFC0108703), the Natural Science
Foundation of Fujian Province of China (2018J06018), the Fundamental Research Funds for the Central
Universities (20720180056), and the Science and
Technology Program of Xiamen
(3502Z20183053) .
The correspondence should be sent to Dr.
Xiaobo Qu (Email: quxiaobo@xmu.edu.cn)
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