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Abstract
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Exact conformal field theories (CFTs) are obtained by using the approach of
Poisson-Lie (PL) T-duality in the presence of spectators.
We explicitly construct some
non-Abelian T-dual $\sigma$-models (here as the PL T-duality on a semi-Abelian double) on $2+2$-dimensional
target manifolds $M \approx O \times \bf G$ and
${\tilde M} \approx O \times {\bf {\tilde G}}$, where $\bf G$ and ${\bf {\tilde G}}$ as two-dimensional
real non-Abelian and Abelian Lie groups act freely on $M$ and $\tilde M$, respectively, while $O$ is the orbit of $\bf G$ in $M$.
The findings of our study show that the original models are equivalent to
Wess-Zumino-Witten (WZW) models based on the Heisenberg $(H_4)$
and $GL(2,\mathbb{R})$ Lie groups. In this way, some new T-dual backgrounds for
these WZW models are obtained. For one of the duals of the $H_4$ WZW model, we show that the model is self-dual.
In the case of the $GL(2,\mathbb{R})$ WZW model it is observed that
the duality transformation changes the asymptotic behavior of solutions from $AdS_{3} \times \mathbb{R}$ to flat space.
Then, the structure and asymptotic nature of the dual
spacetime of this model including the horizon and singularity are determined.
We furthermore get the non-critical
Bianchi type III string cosmological model with a non-vanishing field strength from T-dualizable $\sigma$-models
and show that this model describes an exact CFT (equivalent to the $GL(2,\mathbb{R})$ WZW model).
After that, the conformal invariance of T-dual models up to two-loop order (first order in $\alpha'$) is discussed.
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