I. Introduction
The acquired magnetic resonance spectroscopic (MRS) signal in -space can be expressed as s({\bm k},t) = \int\!\!\!\!\int \rho ({\bm r},f) e^{-i 2 \pi {\bm k} \cdot {\bm r}} e^{-i 2 \pi ft} d {\bm r} df + \xi ({\bm k},t) \eqno{\hbox{(1)}}
where denotes the desired spatial-spectral function and is the measurement noise often modeled as a complex white Gaussian process. The function provides valuable information on the spatial-spectral distribution of metabolites, and is useful for noninvasive metabolite imaging of living systems. For example, 13C magnetic resonance spectroscopic imaging (MRSI) can be used to study glucose metabolism [1]; 31P MRSI is capable of detecting metabolites participating in tissue energy metabolism [1]; 1H MRSI can map out the spatial distributions of N-Acetylaspartate (NAA), creatine, choline, and lactate metabolites that are useful for the investigation of neurological disorders [2]. However, considerable practical challenges remain in obtaining in both high spatial-spectral resolution and high signal-to-noise ratio (SNR). These difficulties are due to acquisition time limitations and low concentrations of metabolites (typically thousands fold below that of tissue water [3]). This paper addresses the low SNR problem.