A generalized Sylvester equation and discrete Ablowitz–Kaup–Newell–Segur type equations

A generalized Sylvester equation is introduced to revisit the Cauchy matrix schemes of the discrete negative-order Ablowitz–Kaup–Newell–Segur (AKNS) equation and the discrete third-order AKNS equation. Starting from the generalized Sylvester equation, we introduce a master function $$\boldsymbol{S}^{(i,j)}$$ that admits a recurrence relation under a constraint relation. By imposing the shifts on matrices $$\boldsymbol{r}$$ and $$\,^\mathrm{t}\! {\boldsymbol{s}}$$ , the shifts of the master function $$\boldsymbol{S}^{(i,j)}$$ are derived. By introducing the dependent variables, the above two discrete AKNS equations are constructed as closed forms. For two different choices of the coefficient matrices in the Sylvester equation that preserve the constraint condition, exact solutions in asymmetric and symmetric cases are presented, with one-soliton, two-soliton, and the simplest Jordan-block solutions given explicitly. Continuum limits to the semidiscrete and continuous AKNS-type equations as well as the corresponding exact solutions are also discussed.

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Publication Details

Journal
Theoretical and Mathematical Physics
Published
2025-05-01
DOI
https://doi.org/10.1134/s004057792505006x
Primary Topic
Fractional Differential Equations Solutions
Type
article
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article

A generalized Sylvester equation and discrete Ablowitz–Kaup–Newell–Segur type equations

Song‐lin Zhao, Shoufeng Shen, Yang Hu
Theoretical and Mathematical Physics
Fractional Differential Equations Solutions
article

A generalized Sylvester equation and discrete Ablowitz–Kaup–Newell–Segur type equations

Song‐lin Zhao, Shoufeng Shen, Yang Hu
article en

Abstract

A generalized Sylvester equation is introduced to revisit the Cauchy matrix schemes of the discrete negative-order Ablowitz–Kaup–Newell–Segur (AKNS) equation and the discrete third-order AKNS equation. Starting from the generalized Sylvester equation, we introduce a master function $$\boldsymbol{S}^{(i,j)}$$ that admits a recurrence relation under a constraint relation. By imposing the shifts on matrices $$\boldsymbol{r}$$ and $$\,^\mathrm{t}\! {\boldsymbol{s}}$$ , the shifts of the master function $$\boldsymbol{S}^{(i,j)}$$ are derived. By introducing the dependent variables, the above two discrete AKNS equations are constructed as closed forms. For two different choices of the coefficient matrices in the Sylvester equation that preserve the constraint condition, exact solutions in asymmetric and symmetric cases are presented, with one-soliton, two-soliton, and the simplest Jordan-block solutions given explicitly. Continuum limits to the semidiscrete and continuous AKNS-type equations as well as the corresponding exact solutions are also discussed.

Theoretical and Mathematical PhysicsVol. 223(2)
Zhejiang University of Technology (CN)
Openalex Percentile: Top 87%
Fractional Differential Equations Solutions
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A generalized Sylvester equation and discrete Ablowitz–Kaup–Newell–Segur type equations — Song‐lin Zhao, Shoufeng Shen, et al. · Theoretical and Mathematical Physics (2025) | TGRS Research Map | TGRS