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SU(2)_0 and OSp(2|2)_{-2} WZNW models : Two current algebras, one Logarithmic CFT
High Energy Physics - Theory · Submitted 19 Jul 2001
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We show that the SU(2)_0 WZNW model has a hidden OSp(2|2)_{-2} symmetry.
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The abstract, sentence by sentence
We show that the SU(2)_0 WZNW model has a hidden OSp(2|2)_{-2} symmetry. Both these theories are known to have logarithms in their correlation functions. We also show that, like OSp(2|2)_{-2}, the logarithmic structure present in the SU(2)_0 model is due to the underlying c=-2 sector. We also demonstrate that the quantum Hamiltonian reduction of SU(2)_0 leads very directly to the correlation functions of the c=-2 model. We also discuss some of the novel boundary effects which can take place in this model.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We show that the SU(2)_0 WZNW model has a hidden OSp(2|2)_{-2} symmetry. | result 0.91 | 0.94 | 0.77 | asserted 1.00 |
| s1 | Both these theories are known to have logarithms in their correlation functions. | background 0.99 | 0.06 | 0.06 | asserted 1.00 |
| s2 | We also show that, like OSp(2|2)_{-2}, the logarithmic structure present in the SU(2)_0 model is due to the underlying c=-2 sector. | result 0.82 | 0.83 | 0.19 | asserted 1.00 |
| s3 | We also demonstrate that the quantum Hamiltonian reduction of SU(2)_0 leads very directly to the correlation functions of the c=-2 model. | result 0.56 | 0.93 | 0.15 | asserted 1.00 |
| s4 | We also discuss some of the novel boundary effects which can take place in this model. | contribution 0.93 | 0.74 | 0.03 | hedged possibility 0.45 |
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Original abstract
We show that the SU(2)_0 WZNW model has a hidden OSp(2|2)_{-2} symmetry. Both these theories are known to have logarithms in their correlation functions. We also show that, like OSp(2|2)_{-2}, the logarithmic structure present in the SU(2)_0 model is due to the underlying c=-2 sector. We also demonstrate that the quantum Hamiltonian reduction of SU(2)_0 leads very directly to the correlation functions of the c=-2 model. We also discuss some of the novel boundary effects which can take place in this model.
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Many 4-point functions are available for such theories, see for instance [ref] .
Exact partition functions for deformed $\mathcal{N}=2$ theories with $N_{f}=4$ flavours · Introduction and results · 0.92
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