<p>In two-dimensional Conformal Field Theory (CFT), multi-stress tensor exchanges between probe operators give rise to the Virasoro identity conformal block, which is fixed by symmetry. The analogous object, and the corresponding organizing principles, in higher dimensions are less well understood. In this paper, we study the Virasoro identity OPE block, which is a bilocal operator that projects two primaries onto the conformal family of multi-stress tensor states. Generalizing a known construction of global OPE blocks, our formalism uses integrals over nested causal diamonds associated with two timelike-separated insertions. We argue that our construction is adaptable to higher dimensions, and use it to provide a new derivation of the single-stress tensor exchange contribution to a four-point correlator in both three and four dimensions, to leading order in the lightcone limit. We also comment on a potential description using effective reparametrization modes in four dimensions.</p>

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Virasoro OPE blocks, causal diamonds, and higher-dimensional CFT

  • Felix M. Haehl,
  • Kuo-Wei Huang

摘要

In two-dimensional Conformal Field Theory (CFT), multi-stress tensor exchanges between probe operators give rise to the Virasoro identity conformal block, which is fixed by symmetry. The analogous object, and the corresponding organizing principles, in higher dimensions are less well understood. In this paper, we study the Virasoro identity OPE block, which is a bilocal operator that projects two primaries onto the conformal family of multi-stress tensor states. Generalizing a known construction of global OPE blocks, our formalism uses integrals over nested causal diamonds associated with two timelike-separated insertions. We argue that our construction is adaptable to higher dimensions, and use it to provide a new derivation of the single-stress tensor exchange contribution to a four-point correlator in both three and four dimensions, to leading order in the lightcone limit. We also comment on a potential description using effective reparametrization modes in four dimensions.