Dual-wavelength noiselike pulses are generated in a fiber ring laser. A first series of pulses is induced at a wavelength of 1550 nm by the interplay of an erbium-doped fiber and nonlinear polarization rotation. From the Raman gain of these pump pulses emerges a second series of Stokes pulses at 1650 nm. With adequate control of the polarization states in the cavity, the noiselike Stokes pulses extend over 84 nm in the Ultralong-wavelengths band (U-band), while the pump pulses span over 46 nm.

We report the first chalcogenide microwire designed with all-normal dispersion to generate supercontinuum by optical wave breaking, a low-noise nonlinear process. The chalcogenide (As2S3) microwire is coated with PMMA and tapered to a diameter of 0.58 μm to achieve the all-normal dispersion regime. The generated supercontinuum spectrum spans over an octave from 960 to >2500  nm using a microwire length of only 3 mm and a low pulse energy of 150 pJ.

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We demonstrate experimentally and numerically the operation of a self-pulsating fiber laser based on the cascaded effects of soliton self-frequency shift and self-phase modulation spectral broadening. The combination of those two effects triggers and sustains the propagation of picosecond pulses in the cavity. At one of the outputs, the laser emits a supercontinuum with spectral width in excess of 150 nm at the repetition rate of 95 kHz.

Self-pulsating sources based on cascaded regeneration by self-phase modulation and offset filtering are investigated experimentally using large filter bandwidths of 3.5 nm and up to semi-infinite bandwidths. In accordance with numerical results reported previously, such sources self-start from amplified spontaneous emission, and picosecond pulses are sustained in a nonlinear cavity. We provide numerical and experimental results indicating the generation of 2 ps pulses and observe 0.4 ps pulses after dispersion compensation and amplification. We also demonstrate that a pair of low- and high-pass filters spawn pulses whose bandwidths are determined by the combination of the filters and gain profiles, hence simplifying the experimental setup for short pulse generation.