Related Experiment Video
Updated: Jun 25, 2026

Low-cost Custom Fabrication and Mode-locked Operation of an All-normal-dispersion Femtosecond Fiber Laser for Multiphoton Microscopy
Published on: November 22, 2019
Dynamics of two laterally coupled semiconductor lasers: strong- and weak-coupling theory
H Erzgräber1, S Wieczorek, B Krauskopf
1School of Engineering, Computing and Mathematics, University of Exeter, Exeter EX4 4QF, United Kingdom.
We investigated coupled semiconductor laser dynamics using three models. A detailed composite-cavity model accurately captures laser coupling, revealing complex dynamics like chaos, unlike simpler models.
Area of Science:
- Optics and Photonics
- Nonlinear Dynamics
- Semiconductor Physics
Background:
- Semiconductor lasers are crucial for modern optics.
- Understanding coupled laser dynamics is essential for advanced applications.
- Evanescent wave coupling is a key mechanism in miniaturized laser systems.
Purpose of the Study:
- To investigate the stability and nonlinear dynamics of side-coupled semiconductor lasers.
- To compare the accuracy of different modeling approaches for coupled laser systems.
- To elucidate the origins of discrepancies between theoretical models.
Main Methods:
- Developed a composite-cavity model considering electric field profiles.
- Performed bifurcation analysis to map system dynamics.
- Introduced phenomenological and derived coupled-laser models.
- Compared dynamics across different modeling approaches.
Main Results:
- The composite-cavity model accurately represents coupling and reveals diverse dynamics (phase-locking, periodic, quasiperiodic, chaotic).
- Individual-laser models with ad hoc terms show significant deviations from the composite-cavity model.
- A derived coupled-laser model aligns with the composite-cavity model under weak coupling.
Conclusions:
- Model choice critically impacts the prediction of coupled semiconductor laser dynamics.
- Accurate modeling requires detailed consideration of the coupled system's electromagnetic field.
- The derived coupled-laser model offers a more physically grounded approach for weak coupling regimes.
Related Concept Videos
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
Biasing of Metal-Semiconductor Junctions
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
¹H NMR: Long-Range Coupling
In alkenes, spin information is communicated via σ–π overlap, as seen in allylic (four-bond) and homoallylic (five-bond) couplings. These coupling interactions are stronger when the σ bond is parallel to the alkene π orbitals.
Spin–Spin Coupling Constant: Overview
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must have a...
Biasing of P-N Junction
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...
Carrier Generation and Recombination
This process is given by the generation rate G and is efficient due to the conservation of momentum between the valence band maximum and conduction band minimum.
Indirect generation involves an...
