“…Theoretically, this theory is of interest because it is an example of a conformal field theory in d > 2 for which explicit expressions for the scaling dimensions of higher-spin operators can be calculated at strong coupling, similar to vector models such as the critical O(N ) model, or the Gross-Neveu model in higher dimensions. (See [5] for a review, and e.g., [6][7][8][9][10][11][12][13][14][15] for calculations of scaling dimensions in vector models related to this paper) or the large flavour limit of 3d QED and QCD (e.g., [16][17][18][19][20][21]). With the revival (e.g., [22][23][24]) of the bootstrap program [25], various interesting methods, results and theorems about higher spin operators, e.g., [26][27][28][29][30][31][32][33] have been developed recently, and comparison to expectations from these analyses is another motivation for this work.…”