M. Zitelli1、*, M. Ferraro1, F. Mangini2, and S. Wabnitz1、3
Author Affiliations
1Department of Information Engineering, Electronics and Telecommunications (DIET), Sapienza University of Rome, 00184 Rome, Italy2Department of Information Engineering (DII), University of Brescia, 25123 Brescia, Italy3Novosibirsk State University, Novosibirsk 630090, Russiashow less
Fig. 1. Simulated energy and wavelength evolution of the three input axial modes. The two upper insets show the pulse power modal distribution at the input (left), and after 1 km of propagation (right).
Fig. 2. Measured output spectra (left column), photodiode traces (center column), and near-field (right column) at 1 km distance, for input pulse peak powers of (a) 2 kW, (b) 6.4 kW, (c) 15 kW, and (d) 110 kW (see Visualization 1).
Fig. 3. Top: Measured wavelength for the three generated solitons versus input peak power. Bottom: corresponding soliton bandwidth evolution.
Fig. 4. Measured beam waist at 1 km distance versus input peak power, when the input beam is coupled with 0°, 2.3°, and 4.6° tilt angle, as compared with the theoretical fundamental mode waist. Input beam waist is 15 μm. Insets show measured output beam shapes at powers indicated by the arrows.
Fig. 5. Measured and simulated FWHM pulse width at 120 m distance versus input peak power. The top insets are autocorrelation traces at 21 kW, 28 kW, and 109 kW input power, respectively.
Fig. 6. Measured bandwidth versus input peak power, for the two solitons observed after 120 m of GRIN fiber.
Fig. 7. Near-field beam waist versus input peak power, for the first soliton at 120 m of GRIN fiber length.
Fig. 8. Recorded autocorrelation traces (left column) and near-field beams (right column) from 120 m of GRIN fiber, for input peak powers: (a) 22 kW, (b) 29 kW, (c) 37 kW, and (d) 109 kW.