Form-factor formulas for partial zero modes in GL(N)-invariant models

Let Tij(1)[0]T^{(1)}_{ij}[0] be the partial zero modes in a GL(N){\rm GL}(N)-invariant model. Bethe vectors and dual Bethe vectors are parametrized by sets tˉk\bar t^k and cardinalities aka_k, and let αk(t)=λk(1)(t)/λk+1(1)(t)\alpha_k(t)=\lambda_k^{(1)}(t)/\lambda_{k+1}^{(1)}(t) for k=1,,N1k=1,\dots,N-1. For a set of κ\kappa-twisted on-shell Bethe parameters tˉ(κˉ)\bar t(\bar\kappa), assume tˉ(κˉ)=tˉ\bar t(\bar\kappa)=\bar t when κˉ=1\bar\kappa=1. The universal form factor of the total operator Tij(z)T_{ij}(z) is denoted by Faˉ(i,j)(sˉ;tˉ){\mathfrak{F}}_{\bar a}^{(i,j)}(\bar s;\bar t). Form-factor conjecture. Form factors of the partial zero modes are given by

Cbˉ(sˉ)Tij(1)[0]Baˉ(tˉ)=(k=1N1αk(sˉk)αk(tˉk)1)Faˉ(i,j)(sˉ;tˉ),forsˉtˉ\mathbb{C}_{\bar b}(\bar s) T^{(1)}_{ij}[0] \mathbb{B}_{\bar a}(\bar t) = \left(\prod_{k=1}^{N-1}\frac{\alpha_k(\bar s^{k})}{\alpha_k(\bar t^{k})}-1\right){\mathfrak{F}}_{\bar a}^{(i,j)}(\bar s;\bar t), \qquad \text{for}\quad \bar s \neq\bar t

and

Caˉ(tˉ)Tii(1)[0]Baˉ(tˉ)=(λi(1)[0]+k=1N1ddκilogαk(tˉk(κˉ))κˉ=1)Baˉ(tˉ)2.\mathbb{C}_{\bar a}(\bar t) T^{(1)}_{ii}[0] \mathbb{B}_{\bar a}(\bar t) = \left( \lambda^{(1)}_{i}[0]+\sum_{k=1}^{N-1}\frac{d}{d\kappa_i} \log\alpha_k\big(\bar t^{k}(\bar\kappa)\big) \Bigr|_{\bar\kappa=1}\right)\|\mathbb{B}_{\bar a}(\bar t)\|^2.

These formulas would extend the form-factor results from GL(3){\rm GL}(3)-invariant models to GL(N){\rm GL}(N) models. The candidate is presented without evidence of resolution, so its status remains open.

Sources & referencesView supporting material

Primary source

Stanislav Pakuliak, Eric Ragoucy and Nikita A. Slavnov, “GL(3)-Based Quantum Integrable Composite Models. II. Form Factors of Local Operators”, arXiv:1502.01966 (2015).

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