Asbtract The feasibility to achieve large-scale spectral compression of an all-normal dispersion fiber laser in a dispersion-increasing fiber is studied both numerically and experimentally. Experimentally, a record-high spectral compression ratio of 46.7 is achieved.
IntroductionIn spectroscopic applications, laser sources with high spectral brightness (power density) are essential in enhancing the signal-to-noise ratio and the reduction of the measurement time. However, typical fs and supercontinuum sources suffer from low spectral brightness due to their inherent wide bandwidth. An interesting solution is to perform external laser spectral compression to effectively enhance the spectral brightness through the redistribution of the energy into a narrow user-desired spectral window. Such spectral narrowing effect was first explained for a negatively-chirped optical pulse propagating in a normal dispersion optical fiber [1]. Chirped optical pulses within standard single-mode fiber [2] and photonic crystal fiber [3,4] were also capable of achieving spectral compression with a moderate spectral compression ratio (below 7). A comb-profiled fiber was used to demonstrate quasi-adiabatic soliton spectral compression [5]. On the other hand, true adiabatic soliton spectral compression using a dispersion-increasing fiber (DIF) was experimentally demonstrated using a soliton fiber laser [6]. Recently, the waveform dependence (parabolic pulses) over the spectral compression ratio within a normal dispersive photonic crystal fiber was addressed [3]. In this paper, we first present numeical analysis on the feasibility in achieving largescale spectral compression ratio within a DIF with linear dispersion ramp. Spectral compressions using same input full-width half-maximum (FWHM) pulse duration, but different waveforms such as sech, Gaussian, parabolic, and dissipative soliton derived from an all-normal dispersion (ANDi) laser [7] are compared. Our numerical results indicate that the ANDi laser can provide the largest compression ratio (greater than 40). Moreover, such large-scale spectral compressions are independent of the signs of the initial pulse chirp applied to input pulses. Experimentally, a record-high spectral compression ratio of 46.7 achieved by launching 160 fs positively-chirped ANDi laser pulses into a DIF.