SCOAP3 Repository 5 records found  Search took 0.22 seconds. 
1. Higher spin currents in the enhanced N = 3 $$ \mathcal{N}=3 $$ Kazama-Suzuki model / Ahn, Changhyun ; Kim, Hyunsu
The N = 3 $$ \mathcal{N}=3 $$ Kazama-Suzuki model at the ‘critical’ level has been found by Creutzig, Hikida and Ronne. [...]
Published in JHEP 1612 (2016) 001 10.1007/JHEP12(2016)001 arXiv:1607.00728
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2. Three point functions in the large N = 4 $$ \mathcal{N}=4 $$ holography / Ahn, Changhyun ; Kim, Hyunsu
Sixteen higher spin currents with spins 1 3 2 3 2 2 $$ \left(1,\frac{3}{2},\frac{3}{2},2\right) $$ , 3 2 2 2 5 2 $$ \left(\frac{3}{2},2,2,\frac{5}{2}\right) $$ , 3 2 2 2 5 2 $$ \left(\frac{3}{2},2,2,\frac{5}{2}\right) $$ , and 2 5 2 5 2 3 $$ \left(2,\frac{5}{2},\frac{5}{2},3\right) $$ were previously obtained in an extension of the large N = 4 $$ \mathcal{N}=4 $$ ‘nonlinear’ superconformal algebra in two dimensions. [...]
Published in JHEP 1510 (2015) 111 10.1007/JHEP10(2015)111 arXiv:1506.00357
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3. Higher spin currents in Wolf space for generic N / Ahn, Changhyun ; Kim, Hyunsu
We obtain the 16 higher spin currents with spins 1 3 2 3 2 2 $$ \left(1,\frac{3}{2},\frac{3}{2},2\right) $$ , 3 2 2 2 5 2 $$ \left(\frac{3}{2},2,2,\frac{5}{2}\right) $$ , 3 2 2 2 5 2 $$ \left(\frac{3}{2},2,2,\frac{5}{2}\right) $$ and 2 5 2 5 2 3 $$ \left(2,\frac{5}{2},\frac{5}{2},3\right) $$ in the N = 4 $$ \mathcal{N}=4 $$ superconformal Wolf space coset S U N + 2 S U N × S U 2 × U 1 $$ \frac{\mathrm{SU}\left(N+2\right)}{\mathrm{SU}(N)\times \mathrm{S}\mathrm{U}(2)\times \mathrm{U}(1)} $$ . [...]
Published in JHEP 1412 (2014) 109 10.1007/JHEP12(2014)109 arXiv:1411.0356
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4. Erratum: Spin-5 Casimir operator its three-point functions with two scalars / Changhyun Ahn ; Hyunsu Kim
Published in JHEP 1401 (2014) 174 10.1007/JHEP01(2014)174
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5. Spin-5 Casimir operator its three-point functions with two scalars / Changhyun Ahn ; Hyunsu Kim
By calculating the second-order pole in the operator product expansion (OPE) between the spin-3 Casimir operator and the spin-4 Casimir operator known previously, the spin-5 Casimir operator is obtained in the coset model based on $ \left( {A_{N-1}^{(1)}\oplus A_{N-1}^{(1) },\ A_{N-1}^{(1) }} \right) $ at level ( k, 1). [...]
Published in JHEP 1401 (2014) 012 10.1007/JHEP01(2014)012 arXiv:1308.1726
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