We propose an all-fiber-generated dual-soliton pulses based scheme for the background-free detection of coherent anti-Stokes Raman spectroscopy under the spectral focusing mechanism. Due to the strong birefringence and high nonlinearity of a polarization-maintaining photonic crystal fiber (PM-PCF), two redshifted soliton pulses can be simultaneously generated relying on high-order dispersion and nonlinear effects along two eigenpolarization axes in the anomalous dispersion regime, while allowing feasible tunability of the frequency distance and temporal interval between them. This proposed scheme, termed as DS-CARS, exploits a unique combination of slight frequency-shift and advisable temporal walk-off of this two soliton pulses to achieve robust and efficient suppression of nonresonant background with compact all-fiber coherent excitation source. Capability of the DS-CARS is experimentally demonstrated by the background-free CARS spectroscopy and unambiguous CARS microscopy of polymer beads in the fingerprint region.Key Words: Spectroscopy, coherent anti-Stokes Raman scattering; Nonlinear microscopy; Pulse propagation and temporal solitons.In the last decade, coherent anti-Stokes Raman scattering (CARS) microscopy has being used increasingly as a unique microscopic tool in biophysics, biology and material sciences [1][2][3]. However, a background from nonresonant (NR) CARS contributions, carrying no chemically specific information severely limits its sensitivity and specificity. The NR background can further distort and even overwhelm the resonant signal of interest, especially in the fingerprint spectral region where molecules present their unique vibrational signature with lower cross section than the frequently used C-H stretch [2]. Several methods have been explored to overcome this problem including phase-and polarization control CARS [4], time-resolved CARS [5], Fourier transform CARS [6], heterodyne interferometric CARS [7] and frequency modulation CARS (FM-CARS) [8,9]. In particular FM-CARS technique has demonstrated its efficient suppression of NR CARS background. However, the reported implementations require hardware modification to provide a second pump laser [8] or modulation of the time delay in the spectral focusing scheme, yielding a complex and costly setup [9]. In addition to the NR background, the complexity of the excitation sources also prevents a broader use of CARS microscopy. The current gold-standard laser system for CARS microscopy is synchronized picosecond (ps) mode-locked solid-state oscillators [10], or synchronously pumped ps OPOs [11]. Free space lasers generally require a stable environment or active feedback, whereas an all-fiber source could be used in less favorable environments while being more compact and inexpensive. Recently, Er-and Yb-doped fiber lasers combined with highly nonlinear fiber or PCF have been put to use in a new type of all-fiber-optic coherent Raman microscopy [12]. Meanwhile, transform-limited (TL) output femtosecond pulses can also be achieved by taking a...