I. Introduction
The exponential function is a basic signal form in signal processing. In many practical applications, signals can be approximated by the superposition of a few exponential functions. Examples include antenna signals in telecommunication [1]–[3], images in fluorescence microscopy [4], analog-to-digital conversion in electronic systems [5], signal functions in the theory of the finite rate of innovation [6], planar polygon recovering [7], and time-domain signals in biological nuclear magnetic resonance (NMR) spectroscopy [8]–[14]. Thus, achieving high-quality recovery of the exponential signals has great significance. The signal of interest is modeled as the sum of exponentials as follows: \begin{equation*} x(n\Delta t)=\sum _{j=1}^{J} {\left ({A_{j} e^{i\phi _{j}}}\right)e^{-\frac {n\Delta t}{\tau _{j}}}e^{i2\pi f_{j} n\Delta t}}\tag{1}\end{equation*} where ) is the normalized frequency, ) is the phase, is the amplitude, is the damping factor, is the number of exponentials, , is the data acquisition (also called sampling) interval, and is the index of fully sampled data points in the time domain with . Accordingly, the sampled data can be represented with a vector . By performing the Fourier transform on , one can obtain a full spectrum .