nonlinear-photonics

Layer 1 — Physics24 concepts in this subtree

Photonic-platform non-linear optics — non-linear wave propagation in fibres, planar waveguides, photonic crystals, and micro-ring resonators. Foundational: Kerr 1875 n(I) = n_0 + n_2·I electro-optic / photoelectric non-linearity;…

Fibre Kerr: n(I) = n_0 + n_2 I → self-phase modulation φ_SPM = γ P L_eff
Manley-Rowe 1956: photon-flux conservation in 3-wave mixing ω_1 + ω_2 = ω_3
Bright soliton in anomalous-dispersion fibre: A(z,t) = √P_0 sech(t/T_0) exp(iγP_0 z/2)
SPM max chirp: δω_max = γ P_0 / T_0 at pulse edges (∂/∂t |A|²) for Gaussian pulse
Manley-Rowe photon balance: ΔΦ_1 = ΔΦ_2 = -ΔΦ_3 per 3-wave interaction step
NLSE bright soliton area theorem: P_0 T_0² = |β_2|/γ exactly for N=1 fundamental
OPA coupled-wave ODE: dA_s/dz = i*kappa*A_i^*; variation-of-parameters closed form
FWM gain matrix eigenvalue bound via Gershgorin discs: |lambda| <= |delta|+|g|
Modulation instability linear stability: eigenvalue via Courant-Fischer min-max principle
OPA exponential gain: |A_s(z)| = |A_s(0)|*cosh(|kappa|*z); asymptotic exp(|kappa|*z)/2
FWM matrix eigenvalues: lambda = +-sqrt(delta^2+|g|^2); Gershgorin bound |lambda|<=|delta|+|g|
MI peak gain at K_peak = sqrt(gamma*P); g_max = gamma*P via Courant-Fischer
Zakharov-Shabat 1972 NLS inverse scattering
Kerr effect (Kerr 1875)
Optical solitons (Mollenauer 1980)
Supercontinuum (Ranka 2000)
SPDC (Burnham-Weinberg 1970)
QPM (Armstrong 1962)
SHG (Franken 1961)
Cross-phase (Garmire 1972)
Zakharov-Shabat (1972)
Frequency comb (Hall-Hänsch 2005)
Microcomb (Del'Haye 2007)
FWM (Stolen 1974)
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