Abstract:We propose the notion of q-characters for finite-dimensional representations of quantum affine algebras. It is motivated by our theory of deformed Walgebras.
“…In the limit ε 2 → 0 X w,ν (x) reduces to the Yangian q-characters of finite-dimensional representations of the Yangian Y (g γ ), constructed for finite γ in [60]. In [38] the qcharacters for the quantum affine algebras U q (g γ ) for finite γ's and in [49] for affine γ's are constructed. These correspond to the K-theoretic version of our story in the limit q 2 → 1, q 1 = q finite, which was discussed in [86].…”
Section: The Main Theoremmentioning
confidence: 99%
“…It would be interesting to apply these ideas to topological strings and to topological gravity. On a more mathematical note, let us discuss the relation of our qq-characters to the tdeformation of q-characters of [38], introduced by H. Nakajima in [75,[78][79][80]. His definition is basically the weighted sum of the Poincare polynomials of the H w,γ -fixed loci on M(w, v).…”
We study symmetries of quantum field theories involving topologically distinct sectors of the field space. To exhibit these symmetries we define special gauge invariant observables, which we call the qq-characters. In the context of the BPS/CFT correspondence, using these observables, we derive an infinite set of Dyson-Schwinger-type relations. These relations imply that the supersymmetric partition functions in the presence of Ω-deformation and defects obey the Ward identities of two dimensional conformal field theory and its q-deformations. The details will be discussed in the companion papers.
“…In the limit ε 2 → 0 X w,ν (x) reduces to the Yangian q-characters of finite-dimensional representations of the Yangian Y (g γ ), constructed for finite γ in [60]. In [38] the qcharacters for the quantum affine algebras U q (g γ ) for finite γ's and in [49] for affine γ's are constructed. These correspond to the K-theoretic version of our story in the limit q 2 → 1, q 1 = q finite, which was discussed in [86].…”
Section: The Main Theoremmentioning
confidence: 99%
“…It would be interesting to apply these ideas to topological strings and to topological gravity. On a more mathematical note, let us discuss the relation of our qq-characters to the tdeformation of q-characters of [38], introduced by H. Nakajima in [75,[78][79][80]. His definition is basically the weighted sum of the Poincare polynomials of the H w,γ -fixed loci on M(w, v).…”
We study symmetries of quantum field theories involving topologically distinct sectors of the field space. To exhibit these symmetries we define special gauge invariant observables, which we call the qq-characters. In the context of the BPS/CFT correspondence, using these observables, we derive an infinite set of Dyson-Schwinger-type relations. These relations imply that the supersymmetric partition functions in the presence of Ω-deformation and defects obey the Ward identities of two dimensional conformal field theory and its q-deformations. The details will be discussed in the companion papers.
“…For example, because of lack of space, I have not discussed such important topics as the theory of conformal algebras [K2, K3] and their chiral counterpart, Lie * algebras [BD2]; quantum deformations of vertex algebras [B3,EK,FR]; and the connection between vertex algebras and integrable systems.…”
“…These relations are called T -systems. In the context of representation theory, these relations are the equations satisfied by the qcharacters [16] of Kirillov-Reshetikhin modules of the Yangians, or the associated quantum affine algebra.…”
Section: 2mentioning
confidence: 99%
“…The T -systems [18,21] satisfied by the transfer matrices of the generalized Heisenberg model or the q-characters of quantum affine algebras [16] can be considered as discrete dynamical systems with special initial conditions. More generally, the equations of these systems can be shown [6] to be mutations in an infinite-rank cluster algebra [13].…”
Abstract. We solve the quantum version of the A 1 T -system by use of quantum networks. The system is interpreted as a particular set of mutations of a suitable (infiniterank) quantum cluster algebra, and Laurent positivity follows from our solution. As an application we re-derive the corresponding quantum network solution to the quantum A 1 Q-system and generalize it to the fully non-commutative case. We give the relation between the quantum T -system and the quantum lattice Liouville equation, which is the quantized Y -system.
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