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Yacine Ikhlef1,2, Jesper Lykke Jacobsen3,4,5, Hubert Saleur5,6

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Researchers have extended Liouville conformal field theory to c≤1, proving its consistency. This new theory connects to microscopic loop models and geometric operators, matching vertex operators in the extended theory.

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Area of Science:

  • Theoretical Physics
  • Condensed Matter Physics
  • String Theory

Background:

  • The extension of Liouville conformal field theory (CFT) to central charges c≤1 has been a long-standing problem.
  • Previous research focused on c≥25, leaving the lower central charge regime largely unexplored.
  • A recent proof established the consistency of c≤1 Liouville CFT, including real critical exponents and analytic continuation of three-point coupling formulas.

Purpose of the Study:

  • To interpret the recently established consistent c≤1 Liouville conformal field theory.
  • To connect this theory to microscopic loop models.
  • To analyze the operator algebra and geometric interpretation of specific operators within this framework.

Main Methods:

  • Introduction of a family of geometrical operators.
  • Development and application of an efficient lattice algorithm for computing three-point functions.
  • Comparison of the computed operator algebra with vertex operators in c≤1 Liouville theory.

Main Results:

  • Demonstrated that the consistent c≤1 Liouville CFT can be interpreted via microscopic loop models.
  • Showcased that the introduced geometric operators' algebra precisely matches that of vertex operators V_{α[over ^]} in c≤1 Liouville theory.
  • Provided a geometric interpretation for the limit α[over ^]→0 of V_{α[over ^]}, explaining its non-identity nature despite zero conformal weight.

Conclusions:

  • The study successfully links microscopic loop models to the extended c≤1 Liouville conformal field theory.
  • The geometric operators provide a concrete realization of the vertex operator algebra in this regime.
  • The findings offer new insights into the structure and interpretation of Liouville CFT at low central charges.