We use the lightcone AdS(3) x S-3 x T-4 superstring sigma model with fermions and bosons subject to twisted boundary conditions to find the ground state energy in the semi-classical approximation where effective string tension h and the light-cone momentum L are sent to infinity in such a way that J = L/h is kept fixed. We then analyse the ground state energy of the model by means of the mirror TBA equations for the AdS(3) x S-3 x T-4 superstring in the pure RR background. The calculation is performed for small twist mu with L and h fixed, for large L with mu and h fixed, and for small h with mu and L fixed. In these limits the contribution of the gapless worldsheet modes coming from the T4 bosons and fermions can be computed exactly, and is shown to be proportional to hL/(4L(2) - 1). Comparison with the semi-classical result shows that the TBA equations involve only one Y-0-function for massless excitations but not two as was conjectured before. Some of the results obtained are generalised to the mixed-flux AdS(3) x S-3 x T-4 superstring.
Ground state energy of twisted AdS3 × S3 × T4 superstring and the TBA
Sfondrini, Alessandro
2023
Abstract
We use the lightcone AdS(3) x S-3 x T-4 superstring sigma model with fermions and bosons subject to twisted boundary conditions to find the ground state energy in the semi-classical approximation where effective string tension h and the light-cone momentum L are sent to infinity in such a way that J = L/h is kept fixed. We then analyse the ground state energy of the model by means of the mirror TBA equations for the AdS(3) x S-3 x T-4 superstring in the pure RR background. The calculation is performed for small twist mu with L and h fixed, for large L with mu and h fixed, and for small h with mu and L fixed. In these limits the contribution of the gapless worldsheet modes coming from the T4 bosons and fermions can be computed exactly, and is shown to be proportional to hL/(4L(2) - 1). Comparison with the semi-classical result shows that the TBA equations involve only one Y-0-function for massless excitations but not two as was conjectured before. Some of the results obtained are generalised to the mixed-flux AdS(3) x S-3 x T-4 superstring.File | Dimensione | Formato | |
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