In this work we obtain the exact solution of quantum integrable system associated with the Lie superalgebra
gl(1∣1), both for periodic and for generic open boundary conditions. By means of the fusion technique we derive a closed set of operator identities among the fused transfer matrices. These identities allow us to determine the complete energy spectrum and the corresponding Bethe ansatz equations of the model. Our approach furnishes a systematic framework for studying the spectra of quantum integrable models based on Lie superalgebras, in particular when the
U(1) symmetry is broken. The derivation of the Bethe states from the exact spectrum is also addressed.
In this work we obtain the exact solution of quantum integrable system associated with the Lie superalgebra \mathfrak{gl}(1|1) 𝔤 𝔩 ( 1 | 1 ) , both for periodic and for generic open boundary conditions. By means of the fusion technique we derive a closed set of operator identities among the fused transfer matrices. These identities allow us to determine the complete energy spectrum and the corresponding Bethe Ansatz equations of the model. Our approach furnishes a systematic framework for studying the spectra of quantum integrable models based on Lie superalgebras, in particular when the U(1) U ( 1 ) symmetry is broken. The derivation of the Bethe states from the exact spectrum is also addressed.
This works uses the two dimensional rotational invariant plane in bosonic symmetry protected topological phases with
C2 rotational symmetry in four dimensions to classify the phases and obtain a boundary field theory as well as an anomalous topological order for the phase that is not captured by the group cohomology classification.