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Quantum loop groups for symmetric Cartan matrices

Andrei Neguţ

TL;DR

This work constructs quantum loop groups for general symmetric Cartan matrices by a Drinfeld-double framework, introducing the radical relations $I^{\pm}$ via a perfect Hopf pairing and expressing the positive/negative halves as quotients $U_q^{\pm}(L\mathfrak{g})$. Central to the approach is a shuffle-algebra model: symmetric rational functions $\mathcal{V}^{\pm}$ with wheel constraints define subalgebras $\mathcal{S}^{\pm}$ whose images under $\widetilde{\Upsilon}^{\pm}$ realize $U_q^{\pm}(L\mathfrak{g})$, yielding a nondegenerate pairing with their duals. Distinguished zig-zags and refined selections encode the loop-Serre-type relations via $\rho_Z$, and the authors prove $U_q^{\pm}(L\mathfrak{g})\cong \mathcal{S}^{\pm}$, establishing a concrete, combinatorial presentation of quantum loop groups. The paper then connects these algebraic structures to $K$-theoretic Hall algebras of quivers without loops, showing that the localized nilpotent KHA $K^{\text{nilp}}_{\mathbb{C}^*,\text{loc}}$ realizes the quantum loop group in simply-laced types, with a geometry-adapted shuffle algebra $\mathcal{S}^{+\text{,geom}}$ governing the correspondence. Together, these results provide a unified framework linking quantum loop groups, shuffle algebras, and geometric representation theory via $K$-theoretic Hall algebras.

Abstract

We introduce a quantum loop group associated to a general symmetric Cartan matrix, by imposing just enough relations between the usual generators $\{e_{i,k}, f_{i,k}\}_{i \in I, k \in \mathbb{Z}}$ in order for the natural Hopf pairing between the positive and negative halves of the quantum loop group to be perfect. As an application, we describe the localized K-theoretic Hall algebra of any quiver without loops, endowed with a particularly important $\mathbb{C}^*$ action.

Quantum loop groups for symmetric Cartan matrices

TL;DR

This work constructs quantum loop groups for general symmetric Cartan matrices by a Drinfeld-double framework, introducing the radical relations via a perfect Hopf pairing and expressing the positive/negative halves as quotients . Central to the approach is a shuffle-algebra model: symmetric rational functions with wheel constraints define subalgebras whose images under realize , yielding a nondegenerate pairing with their duals. Distinguished zig-zags and refined selections encode the loop-Serre-type relations via , and the authors prove , establishing a concrete, combinatorial presentation of quantum loop groups. The paper then connects these algebraic structures to -theoretic Hall algebras of quivers without loops, showing that the localized nilpotent KHA realizes the quantum loop group in simply-laced types, with a geometry-adapted shuffle algebra governing the correspondence. Together, these results provide a unified framework linking quantum loop groups, shuffle algebras, and geometric representation theory via -theoretic Hall algebras.

Abstract

We introduce a quantum loop group associated to a general symmetric Cartan matrix, by imposing just enough relations between the usual generators in order for the natural Hopf pairing between the positive and negative halves of the quantum loop group to be perfect. As an application, we describe the localized K-theoretic Hall algebra of any quiver without loops, endowed with a particularly important action.
Paper Structure (5 sections, 28 theorems, 345 equations, 9 figures)

This paper contains 5 sections, 28 theorems, 345 equations, 9 figures.

Key Result

Theorem 1.4

The ideal $I^+$ is generated by the coefficients of the series $\rho_Z$ of eqn:rho intro, as $Z$ goes over all distinguished zig-zags, for any $i \neq j$ in $I$. Thus, the positive half of the quantum loop group may be defined as The negative half $U_q^-(L\mathfrak{g})$ can be defined analogously (with $f_{i,-k}$'s instead of $e_{i,k}$'s).

Figures (9)

  • Figure 1: A distinguished zig-zag $Z$
  • Figure 2: A minimal zig-zag $Z$
  • Figure 3: A particular minimal zig-zag $Z$
  • Figure 4: A zig-zag $Z$ for $d_{ij} = -7$ ($m_Z = 3$)
  • Figure 5: A minimal zig-zag $Z$, for $d_{ij} = -7$, $k=2$, $l=5$
  • ...and 4 more figures

Theorems & Definitions (74)

  • Theorem 1.4
  • Theorem 1.7
  • Theorem 1.8
  • Theorem 1.9
  • Theorem 1.12
  • Definition 1.17
  • Remark 1.19
  • Definition 2.2
  • Definition 2.4
  • Proposition 2.6
  • ...and 64 more