TY - JOUR
T1 - The N = 2 supersymmetric w 1+∞ symmetry in the two-dimensional SYK models
AU - Ahn, Changhyun
N1 - Publisher Copyright:
© 2022, The Author(s).
PY - 2022/5
Y1 - 2022/5
N2 - We identify the rank (qsyk + 1) of the interaction of the two-dimensional N = (2, 2) SYK model with the deformation parameter λ in the Bergshoeff, de Wit and Vasiliev (in 1991)’s linear W∞[λ] algebra via λ=12(qsyk+1) by using a matrix generalization. At the vanishing λ (or the infinity limit of qsyk), the N = 2 supersymmetric linear W∞N,N[λ = 0] algebra contains the matrix version of known N = 2 W∞ algebra, as a subalgebra, by realizing that the N-chiral multiplets and the N-Fermi multiplets in the above SYK models play the role of the same number of βγ and bc ghost systems in the linear W∞N,N[λ = 0] algebra. For the nonzero λ, we determine the complete N = 2 supersymmetric linear W∞N,N[λ] algebra where the structure constants are given by the linear combinations of two different generalized hypergeometric functions having the λ dependence. The weight-1,12 currents occur in the right hand sides of this algebra and their structure constants have the λ factors. We also describe the λ = 14 (or qsyk = 1) case in the truncated subalgebras by calculating the vanishing structure constants.
AB - We identify the rank (qsyk + 1) of the interaction of the two-dimensional N = (2, 2) SYK model with the deformation parameter λ in the Bergshoeff, de Wit and Vasiliev (in 1991)’s linear W∞[λ] algebra via λ=12(qsyk+1) by using a matrix generalization. At the vanishing λ (or the infinity limit of qsyk), the N = 2 supersymmetric linear W∞N,N[λ = 0] algebra contains the matrix version of known N = 2 W∞ algebra, as a subalgebra, by realizing that the N-chiral multiplets and the N-Fermi multiplets in the above SYK models play the role of the same number of βγ and bc ghost systems in the linear W∞N,N[λ = 0] algebra. For the nonzero λ, we determine the complete N = 2 supersymmetric linear W∞N,N[λ] algebra where the structure constants are given by the linear combinations of two different generalized hypergeometric functions having the λ dependence. The weight-1,12 currents occur in the right hand sides of this algebra and their structure constants have the λ factors. We also describe the λ = 14 (or qsyk = 1) case in the truncated subalgebras by calculating the vanishing structure constants.
KW - Conformal and W Symmetry
KW - Higher Spin Symmetry
UR - http://www.scopus.com/inward/record.url?scp=85130414939&partnerID=8YFLogxK
U2 - 10.1007/JHEP05(2022)115
DO - 10.1007/JHEP05(2022)115
M3 - Article
AN - SCOPUS:85130414939
SN - 1029-8479
VL - 2022
JO - Journal of High Energy Physics
JF - Journal of High Energy Physics
IS - 5
M1 - 115
ER -