Higher Spin Currents in the Holographic N=1 Coset Minimal Model
arXiv:1310.6185 · doi:10.1007/JHEP01(2014)007
Abstract
In the N=1 supersymmetric coset minimal model based on (B_N^{(1)} \oplus D_N^{(1)}, D_N^{(1)}) at level (k,1) studied recently, the standard N=1 super stress tensor of spins (3/2,2) is reviewed. By considering the stress tensor in the coset (B_N^{(1)}, D_N^{(1)}) at level k, the higher spin-2' Casimir current was obtained previously. By acting the above spin-3/2 current on the higher spin-2' Casimir current, its superpartner, the higher spin-5/2 current, can be generated and combined as the first higher spin supercurrent with spins (2', 5/2). By calculating the operator product expansions (OPE) between the higher spin supercurrent and itself, the next higher spin supercurrent can be generated with spins (7/2,4). Moreover, the other higher spin supercurrent with spins (4',9/2) can be generated by calculating the OPE between the first higher spin supercurrent with spins (2', 5/2) and the second higher spin supercurrent with spins (7/2,4). Finally, the higher spin supercurrent, (11/2,6), can be extracted from the right hand side of OPE between the higher spin supercurrents, (2', 5/2) and (4', 9/2).
97 pages; footnotes 1, 7 and 9 and the last paragraph of Appendix F added and to appear in JHEP
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- Higher Spin Currents in Wolf Space for Generic N
- Higher Spin Currents in Orthogonal Wolf Space
- Higher Spin Currents in the Enhanced N=3 Kazama-Suzuki Model
- The Next Higher Spin Currents and Three-Point Functions in the Large Holography
- Three Point Functions in the N=4 Orthogonal Coset Theory
- Higher Spin Currents in the Orthogonal Coset Theory
- A Supersymmetric Enhancement of Holographic Minimal Model
- Adding Complex Fermions to the Grassmannian-like Coset Model
- The Operator Product Expansions in the Orthogonal Wolf Space Coset Model
- Higher Spin Currents with Manifest Symmetry in the Large Holography