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Generating twisted Cherednik eigenfunctions

A. Mironov, A. Morozov, A. Popolitov

Abstract

Hamiltonians ${\cal H}^{a}_k$ of new integrable systems associated with the integer rays $(1,a)$ (commutative subalgebras) of Ding-Iohara-Miki (DIM) algebra in the $N$-body representation are closely related to commuting twisted Cherednik Hamiltonians $\mathfrak{C}_i^{(a)}$, ${\cal H}^{a}_k = \sum_{i=1}^N (\mathfrak{C}_i^{(a)})^k$. Moreover, symmetric combinations of eigenfunctions in the twisted Cherednik system were recently shown to produce the DIM Hamiltonian eigenstates. We explicitly construct these twisted Cherednik eigenfunctions recurrently by action of some (creation and permutation) operations. It resembles of a far-going generalization of Kirillov-Noumi operators, but exact relation remains to be specified.

Generating twisted Cherednik eigenfunctions

Abstract

Hamiltonians of new integrable systems associated with the integer rays (commutative subalgebras) of Ding-Iohara-Miki (DIM) algebra in the -body representation are closely related to commuting twisted Cherednik Hamiltonians , . Moreover, symmetric combinations of eigenfunctions in the twisted Cherednik system were recently shown to produce the DIM Hamiltonian eigenstates. We explicitly construct these twisted Cherednik eigenfunctions recurrently by action of some (creation and permutation) operations. It resembles of a far-going generalization of Kirillov-Noumi operators, but exact relation remains to be specified.
Paper Structure (28 sections, 60 equations, 1 figure)

This paper contains 28 sections, 60 equations, 1 figure.

Figures (1)

  • Figure 1: $2d$ integer lattice of generators of the elliptic Hall/DIM algebra. Each ray (p,r) gives rise to a commutative subalgebra, and each pair of rays (p,r) and (-p,-r) form a Heisenberg subalgebra.