- Parametric amplification
- Wavelength conversion
- Pulse compression
- Supercontinuum source
- Light regenerator
- Discrete type (or lumped type) Raman amplifier
The non-linear effects of optical fibre, such as stimulated Raman scattering (SRS), stimulated Brillouin scattering (SBS), and the optical Kerr effect, find numerous applications in the fields of communications and optical signal processing. In the Kerr effect, the refractive index of optical dielectric materials changes with optical power, triggering a series of secondary effects, such as self-phase modulation (SPM), cross phase modulation (XPM), four-wave mixing (FWM), and non-steady state modulation. The Kerr effect finds applications in optical parametric amplification, frequency conversion, phase coupling, pulse compression and generation, as well as optical soliton transmission.
When designing the high nonlinear optical fibre (HNLF), considerations shall include the following: First, ensure a higher nonlinear coefficient for sufficient non-linear effect. Second, ensure lower loss to increase the effective length (Leff). Third, align dispersion characteristics to cater to different applications. Finally, maintain low polarization mode dispersion (PMD) in the optical fibre. For silica-based HNLF, the design of the refractive index profile plays an important role in order to meet the aforementioned requirements. In the design of HNLF, it is essential to simultaneously implement a small core effective area (Aeff), a low dispersion slope, and much smaller cut-off wavelengths than the operating wavelength.
The HNLF is independently developed and produced by YOFC, featuring a high nonlinear coefficient and a very low dispersion slope. With a flexible W-type profile design, an inner cladding with a low refractive index is set around the step-index core.


| Fibre type | NL 1550-POS | NL 1550-Zero | NL 1550-NEG |
|---|---|---|---|
| Part No. | NL1016-A | NL1016-B | NL1016-C |
| Optical properties | |||
| Operating wavelength | C-Band | C-Band | C-Band |
| Dispersion slope @1550 nm (ps/nm²·km) | <0.035 | <0.035 | <0.035 |
| Dispersion @1550 nm (ps/nm·km) | >1 | 0.0±1 | <-1 |
| Nonlinear coefficient @1550 nm (W⁻¹km⁻¹) | ≥10 | ≥10 | ≥10 |
| Attenuation Coefficient @1550nm (dB/km) | ≤1.5 | ≤1.5 | ≤1.5 |
| Fibre cutoff wavelength (nm) | <1480 | <1480 | <1480 |
| NA (typical value) | 0.35 | 0.35 | 0.35 |
| Geometrical properties | |||
| Cladding diameter (μm) | 125.0±5.0 | 125.0±5.0 | 125.0±5.0 |
| Cladding non-circularity (%) | ≤1.0 | ≤1.0 | ≤1.0 |
| Core/Cladding concentricity error (μm) | ≤0.5 | ≤0.5 | ≤0.5 |
| Coating diameter (μm) | 245.0±10.0 | 245.0±10.0 | 245.0±10.0 |