Transport in simple networks described by integrable discrete nonlinear Schr\"Aodinger equation
K. Nakamura, Z.A. Sobirov, D.U. Matrasulov, S. Sawada

TL;DR
This paper demonstrates that the Ablowitz-Ladik discrete nonlinear Schrödinger equation on simple networks remains integrable, with solutions related to 1D AL solitons, under specific nonlinearity conditions, leading to conserved quantities and predictable transmission.
Contribution
It extends the integrability of the AL discrete NLSE from 1D chains to simple network structures with bond-dependent nonlinearities, identifying conditions for solutions and conservation laws.
Findings
Solutions are bond-dependent AL solitons scaled by nonlinearity
Nonlinearity sum rule at network vertices ensures integrability
Transmission probabilities are inversely proportional to nonlinearity strength
Abstract
We elucidate the case in which the Ablowitz-Ladik (AL) type discrete nonlinear Schr\"Aodinger equa- tion (NLSE) on simple networks (e.g., star graphs and tree graphs) becomes completely integrable just as in the case of a simple 1-dimensional (1-d) discrete chain. The strength of cubic nonlinearity is different from bond to bond, and networks are assumed to have at least two semi-infinite bonds with one of them working as an incoming bond. The present work is a nontrivial extension of our preceding one (Sobirov et al, Phys. Rev. E 81, 066602 (2010)) on the continuum NLSE to the discrete case. We find: (1) the solution on each bond is a part of the universal (bond-independent) AL soliton solution on the 1-d discrete chain, but is multiplied by the inverse of square root of bond-dependent nonlinearity; (2) nonlinearities at individual bonds around each vertex must satisfy a sum rule; (3)…
Peer Reviews
No public reviews on file for this paper yet. If you reviewed it on a platform where reviews are public (OpenReview, ICLR, NeurIPS, ICML), you can paste yours below so the community can read it here.
Videos
No videos yet. Explain this paper in a talk, walkthrough, or lecture? Add one.
