scholarly journals Construction of Arbitrary Order Conformally Invariant Operators in Higher Spin Spaces

2017 ◽  
Vol 27 (3) ◽  
pp. 2418-2452 ◽  
Author(s):  
Chao Ding ◽  
Raymond Walter ◽  
John Ryan
1988 ◽  
Vol 300 ◽  
pp. 637-657 ◽  
Author(s):  
M. Baake ◽  
P. Christe ◽  
V. Rittenberg

2006 ◽  
Vol 18 (08) ◽  
pp. 823-886 ◽  
Author(s):  
O. V. SHAYNKMAN ◽  
I. YU. TIPUNIN ◽  
M. A. VASILIEV

A constructive procedure is proposed for formulation of linear differential equations invariant under global symmetry transformations forming a semi-simple Lie algebra 𝔣. Under certain conditions, 𝔣-invariant systems of differential equations are shown to be associated with 𝔣-modules that are integrable with respect to some parabolic subalgebra of 𝔣. The suggested construction is motivated by the unfolded formulation of dynamical equations developed in the higher spin gauge theory and provides a starting point for generalization to the nonlinear case. It is applied to the conformal algebra 𝔬(M, 2) to classify all linear conformally invariant differential equations in the Minkowski space. Numerous examples of conformal equations are discussed from this perspective.


2014 ◽  
Vol 55 (10) ◽  
pp. 101703 ◽  
Author(s):  
D. Eelbode ◽  
T. Raeymaekers

2015 ◽  
Vol 31 (1) ◽  
pp. 303-312
Author(s):  
Paolo Mastrolia ◽  
Dario Monticelli

2021 ◽  
Vol 2021 (9) ◽  
Author(s):  
Sachin Jain ◽  
Renjan Rajan John ◽  
Abhishek Mehta ◽  
Amin A. Nizami ◽  
Adithya Suresh

Abstract In this paper we use the spinor-helicity formalism to calculate 3-point functions involving scalar operators and spin-s conserved currents in general 3d CFTs. In spinor-helicity variables we notice that the parity-even and the parity-odd parts of a correlator are related. Upon converting spinor-helicity answers to momentum space, we show that correlators involving spin-s currents can be expressed in terms of some simple conformally invariant conserved structures. This in particular allows us to understand and separate out contact terms systematically, especially for the parity-odd case. We also reproduce some of the correlators using weight-shifting operators.


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