Non-Wilson-Fisher kinks of numerical bootstrap: from the deconfined phase transition to a putative new family of CFTs
arXiv:2005.04250 · doi:10.21468/SciPostPhys.10.5.115
Abstract
It is well established that the Wilson-Fisher (WF) CFT sits at a kink of the numerical bounds from bootstrapping four point function of vector. Moving away from the WF kinks, there indeed exists another family of kinks (dubbed non-WF kinks) on the curve of numerical bounds. Different from the WF kinks that exist for arbitary in dimensions, the non-WF kinks exist in arbitrary dimensions but only for a large enough in a given dimension . In this paper we have achieved a thorough understanding for few special cases of these non-WF kinks. The first case is the bootstrap in 2d, where the non-WF kink turns out to be the Wess-Zumino-Witten (WZW) model, and all the WZW models saturate the numerical bound on the left side of the kink. We further carry out dimensional continuation of the 2d kink towards the 3d deconfined phase transition. We find the kink disappears at around dimensions indicating the deconfined phase transition is weakly first order. The second interesting observation is, the bootstrap bound does not show any kink in 2d (), but is surprisingly saturated by the 2d free boson CFT (also called Luttinger liquid) all the way on the numerical curve. The last case is the limit, where the non-WF kink sits at in dimensions. We manage to write down its analytical four point function in arbitrary dimensions, which equals to the subtraction of correlation functions of a free fermion theory and generalized free theory. An important feature of this solution is the existence of a full tower of conserved higher spin current. We speculate that a new family of CFTs will emerge at non-WF kinks for finite , in a similar fashion as WF CFTs originating from free boson at .
16+3 pages
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