TY - JOUR
T1 - The full Quantum Spectral Curve for $AdS_4/CFT_3$
AU - Bombardelli, Diego
AU - Cavaglià, Andrea
AU - Fioravanti, Davide
AU - Gromov, Nikolay
AU - Tateo, Roberto
N1 - 41 pages + 5 Appendices, 7 figures. v3: text improved, typos fixed, references added, more details in Appendix A
PY - 2017/9/27
Y1 - 2017/9/27
N2 - The spectrum of planar N=6 superconformal Chern-Simons theory, dual to type IIA superstring theory on $AdS_4 \times CP^3$, is accessible at finite coupling using integrability. Starting from the results of [arXiv:1403.1859], we study in depth the basic integrability structure underlying the spectral problem, the Quantum Spectral Curve. The new results presented in this paper open the way to the quantitative study of the spectrum for arbitrary operators at finite coupling. Besides, we show that the Quantum Spectral Curve is embedded into a novel kind of Q-system, which reflects the OSp(4|6) symmetry of the theory and leads to exact Bethe Ansatz equations. The discovery of this algebraic structure, more intricate than the one appearing in the $AdS_5/CFT_4$ case, could be a first step towards the extension of the method to $AdS_3/CFT_2$.
AB - The spectrum of planar N=6 superconformal Chern-Simons theory, dual to type IIA superstring theory on $AdS_4 \times CP^3$, is accessible at finite coupling using integrability. Starting from the results of [arXiv:1403.1859], we study in depth the basic integrability structure underlying the spectral problem, the Quantum Spectral Curve. The new results presented in this paper open the way to the quantitative study of the spectrum for arbitrary operators at finite coupling. Besides, we show that the Quantum Spectral Curve is embedded into a novel kind of Q-system, which reflects the OSp(4|6) symmetry of the theory and leads to exact Bethe Ansatz equations. The discovery of this algebraic structure, more intricate than the one appearing in the $AdS_5/CFT_4$ case, could be a first step towards the extension of the method to $AdS_3/CFT_2$.
KW - hep-th
U2 - 10.1007/JHEP09(2017)140
DO - 10.1007/JHEP09(2017)140
M3 - Article
SN - 1126-6708
JO - JHEP
JF - JHEP
ER -