We demonstrate that bright solitons can be generated in a normal-dispersion target band of a multi-zero-dispersion photonic crystal fiber with frequency-dependent nonlinearity. The fiber is pumped at 804 nm and has three zero-dispersion wavelengths at 771, 920, and 1070 nm, while the nonlinear coefficient changes sign at 771 and 920 nm. This creates a four-region dispersion-nonlinearity landscape in which the 920–1070 nm band combines normal dispersion with negative nonlinearity. Using a photon-conserving generalized nonlinear Schrödinger equation, we show that energy transferred from the anomalous-dispersion pump band evolves into a delayed, temporally localized bright soliton in this target band. The generated soliton exhibits a fundamental-like nonlinear-dispersive balance, while the long-wavelength component beyond 1070 nm behaves as dispersive radiation. By varying the input pulse width, we identify a favorable intermediate operating range around 35–40 fs. Within this range, the 35 fs case provides the best balanced target-band output, combining appreciable conversion efficiency, a center wavelength on the long-wavelength side of Region III, and a near-fundamental effective soliton order. These results show that the joint engineering of zero-dispersion and zero-nonlinearity wavelengths can transform a normal-dispersion region into a usable bright-soliton output channel, offering a potential design principle for tunable ultrafast pulse sources, wavelength-conversion schemes, and target-band nonlinear light-source design.
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Peng et al. (2026) studied this question.
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