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Anomalous solutions to the strong CP problem.

Anson Hook1

  • 1School of Natural Sciences, Institute for Advanced Study, Princeton, New Jersey 08540, USA.

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|April 25, 2015
PubMed
Summary
This summary is machine-generated.

This study introduces a novel mechanism to solve the strong CP problem using Z_{2} discrete and anomalous U(1) symmetries. The proposed models predict new colored particles at the TeV scale, offering testable predictions for physics beyond the Standard Model.

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Area of Science:

  • High Energy Physics
  • Particle Physics
  • Theoretical Physics

Background:

  • The strong CP problem is a major unsolved puzzle in the Standard Model of particle physics.
  • Existing solutions often require fine-tuning or introduce new, unobserved particles.
  • Anomalous U(1) symmetries offer a potential framework for addressing this problem.

Purpose of the Study:

  • To propose a new mechanism for solving the strong CP problem.
  • To explore the implications of Z_{2} discrete and anomalous U(1) symmetries in this context.
  • To present concrete, testable predictions for new physics.

Main Methods:

  • Utilizing a Z_{2} discrete symmetry to equate theta angles of two gauge groups.
  • Employing an anomalous U(1) symmetry to render the difference between theta angles physical.
  • Developing two distinct models illustrating the infrared manifestation of the anomalous symmetry.

Main Results:

  • The first model features massless bifundamental quarks, with the η^{'} boson relaxing the QCD theta angle to zero.
  • The second model realizes the anomalous U(1) symmetry as a dynamically generated mass term that cancels the theta angle.
  • Both models predict the existence of new colored particles at the TeV scale.

Conclusions:

  • The proposed mechanism offers a compelling solution to the strong CP problem.
  • The predicted TeV-scale colored particles provide a direct experimental signature for these models.
  • This work opens new avenues for exploring solutions to fundamental problems in particle physics.