Kerr envelopes, dispersion and soliton limits
Research context
postgraduate concept · conditional · As of 2026-10-10
In a lossless scalar narrowband Kerr envelope convention, i∂_zA=−D∂²_tA+δ|A|²A represents second-order dispersion and self-phase modulation.
Key knowledge
In a lossless scalar narrowband Kerr envelope convention, i∂_zA=−D∂²_tA+δ|A|²A represents second-order dispersion and self-phase modulation. The signs and amplitude normalization set which regime supports bright solitons. This reduced model omits higher dispersion, delayed nonlinear response and transverse dynamics; an ideal soliton is not immunity to perturbations.
Values and equations
i∂_zA=−D∂²_tA+δ|A|²A
- A
- Field envelope with |A|² an intensity W½ m⁻¹
- z
- Propagation distance m
- t
- Retarded time s
- D
- Dispersion coefficient in this convention s² m⁻¹
- δ
- Intensity-normalized nonlinear coefficient m W⁻¹
Conditions and scope
- Retarded time t, slowly varying envelope, specified reference carrier and intensity normalization |A|² in W m⁻²; D and δ follow that convention.
- Shorter pulses, Raman/self-steepening, loss, focusing and periodic perturbations require extended equations and independent propagation checks.
Sources · 1
References
Sources retain their recorded scope. A source link alone does not establish verification of every statement.
Evidence and review
Inspected §§3.1–3.3, 3.5–3.6: Kerr response, phase modulation, envelope convention and soliton perturbations; source check dated 2026-10-10. Scope is limited to the cited statements, equations and assumptions, not the whole publication.
2026-10-10 · Author source inspection of the displayed claim, model assumptions and equations; independent exact-content and branch-inventory review is a separate gate. Contemporary status is a dated snapshot, not a promise of ongoing monitoring.
Entry details
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