Yang-Mills as a Liouville theory

Stephan Stieberger (Max–Planck–Institut für Physik, Werner–Heisenberg–Institut, München, Germany) ; Tomasz R. Taylor (Department of Physics, Northeastern University, Boston, USA; Faculty of Physics, University of Warsaw, ul. Pasteura 5, Warsaw, Poland) ; Bin Zhu (School of Mathematics, Maxwell Institute for Mathematical Sciences, University of Edinburgh, UK)

We propose a description of the gluon scattering amplitudes as the inverse Mellin transforms of the conformal correlators of light operators in two-dimensional Liouville theory tensored with WZW-like chiral currents on the celestial sphere. The dimensions of operators are Mellin dual to gluon light cone energies while their positions are determined by the gluon momentum directions. Tree-level approximation in Yang-Mills theory corresponds to the semiclassical limit of Liouville theory. By comparing subleading corrections, we find b2=(8π2)1β0g2(M), where b is the Liouville coupling constant, g(M) is the Yang Mills coupling at the renormalization scale M and β0 is the one-loop coefficient of the Yang-Mills beta function.

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        {
          "country": "Poland", 
          "value": "Faculty of Physics, University of Warsaw, ul. Pasteura 5, Warsaw, Poland"
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      "surname": "Taylor", 
      "email": "taylor@neu.edu", 
      "full_name": "Taylor, Tomasz R.", 
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      "surname": "Zhu", 
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      "full_name": "Zhu, Bin", 
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      "source": "Elsevier", 
      "value": "We propose a description of the gluon scattering amplitudes as the inverse Mellin transforms of the conformal correlators of light operators in two-dimensional Liouville theory tensored with WZW-like chiral currents on the celestial sphere. The dimensions of operators are Mellin dual to gluon light cone energies while their positions are determined by the gluon momentum directions. Tree-level approximation in Yang-Mills theory corresponds to the semiclassical limit of Liouville theory. By comparing subleading corrections, we find <math><msup><mrow><mi>b</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>=</mo><msup><mrow><mo>(</mo><mn>8</mn><msup><mrow><mi>\u03c0</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>)</mo></mrow><mrow><mo>\u2212</mo><mn>1</mn></mrow></msup><msub><mrow><mi>\u03b2</mi></mrow><mrow><mn>0</mn></mrow></msub><mspace width=\"0.2em\"></mspace><msup><mrow><mi>g</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>(</mo><mi>M</mi><mo>)</mo></math>, where b is the Liouville coupling constant, <math><mi>g</mi><mo>(</mo><mi>M</mi><mo>)</mo></math> is the Yang Mills coupling at the renormalization scale M and <math><msub><mrow><mi>\u03b2</mi></mrow><mrow><mn>0</mn></mrow></msub></math> is the one-loop coefficient of the Yang-Mills beta function."
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Published on:
05 October 2023
Publisher:
Elsevier
Published in:
Physics Letters B , Volume 846 C (2023)

Article ID: 138229
DOI:
https://doi.org/10.1016/j.physletb.2023.138229
Copyrights:
The Author(s)
Licence:
CC-BY-3.0

Fulltext files: