Letters in Mathematical Physics· 2026Q1
A $$3\times 3$$ linear q-difference system with $$E_8^{(1)}$$-symmetry
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- 2026year
Short summary
A novel 3x3 linear q-difference equation exhibiting E8(1) affine Weyl group symmetry has been developed, extending existing quantum curves.
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Key points
- A 3x3 linear q-difference equation with E8(1) affine Weyl group symmetry is presented.
- The equation has 8 parameters and 2 accessory parameters, characterized by spectral type.
- It extends Moriyama-Yamada's quantum curve which has W(E8(1))-symmetry.
- Symmetry is achieved via a q-middle convolution, reconstructed through a q-Okubo-type equation.
AI-generated from the title and abstract; the full text is not read.
Abstract
Abstract We present a linear q -difference equation of rank 3, which admits the affine Weyl group symmetry of type $$E_8^{(1)}$$ E 8 ( 1 ) . This equation has essentially 8 parameters and 2 accessory parameters. We characterize this equation by the spectral type of q -difference system which is introduced by Sakai–Yamaguchi. We further compare this equation with Moriyama–Yamada’s quantum curve which has $$W(E_8^{(1)})$$ W ( E 8 ( 1 ) ) -symmetry. We show that our equation can be regarded as an extension of Moriyama–Yamada’s curve. We introduce the point configuration of a higher-order scalar q -difference equation to characterize our equation and clarify the corresponding between our equation and the curve. The symmetry of our equation is provided by the q -middle convolution, defined by Sakai–Yamaguchi and reformulated by Arai–Takemura. In this paper, we provide a reconstruction of the q -middle convolution via a q -Okubo-type equation. This construction is a natural q -analog of the middle convolution of Fuchsian differential equation. Several properties for our q -middle convolution are also discussed.
The authors' abstract, as published at the source. Letters in Mathematical Physics, 2026 · DOI ↗
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Field: Geometry and Topology
Geometry and TopologyMathematics