Phases Of Adjoint QCD_3 And Dualities

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In summary, the paper by Gomis, Komargodski, and Seiberg explores the possible phases of adjoint QCD in 2+1 dimensions by using symmetries, anomalies, and renormalization group flows. They propose a quantum mechanical phase with a Topological Quantum Field Theory description at small Chern-Simons level, and discover a special mass choice that leads to N=1 supersymmetry and the presence of a massless Majorana fermion. The authors also suggest new infrared fermion-fermion dualities and a phase diagram for SO/Sp gauge theories with a fermion in the traceless symmetric/antisymmetric tensor representation, and conjecture the value of the time-reversal anomaly
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David Neves
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Here is an interesting paper where they uncover new dualities by studying adjoint QCD in 2 + 1 dimensions.

https://arxiv.org/pdf/1710.03258.pdfPhases Of Adjoint QCD_3 And Dualities

by Jaume Gomis, Zohar Komargodski, and Nathan Seiberg

We study 2+1 dimensional gauge theories with a Chern-Simons term and a fermion in the adjoint representation. We apply general considerations of symmetries, anomalies, and renormalization group flows to determine the possible phases of the theory as a function of the gauge group, the Chern-Simons level
k, and the fermion mass. We propose an inherently quantum mechanical phase of adjoint QCD with small enough k, where the infrared is described by a certain Topological Quantum Field Theory (TQFT). For a special choice of the mass, the theory has N = 1 supersymmetry. There this TQFT is accompanied by a
massless Majorana fermion – a Goldstino signaling spontaneous supersymmetry breaking. Our analysis leads us to conjecture a number of new infrared fermion-fermion dualities involving SU, SO, and Sp
gauge theories. It also leads us to suggest a phase diagram of SO/Sp gauge theories with a fermion in the traceless symmetric/antisymmetric tensor representation of the gauge group. As a by-product of our analysis, we conjecture the value of the time-reversal anomaly ν of U (n)_n,2n, SO(n)_n, and Sp(n)_n Chern-Simons theories.
 
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Thank you for sharing this interesting paper on the study of adjoint QCD in 2+1 dimensions. I find this research to be particularly intriguing as it uncovers new dualities and provides insights into the possible phases of the theory.

The authors' approach of using symmetries, anomalies, and renormalization group flows to determine the phases of the theory is a rigorous and comprehensive method. Their proposal of an inherently quantum mechanical phase of adjoint QCD with small Chern-Simons level, where the infrared is described by a Topological Quantum Field Theory, is a significant contribution to the field.

Furthermore, the discovery of a special mass choice that leads to N=1 supersymmetry and the presence of a massless Majorana fermion, indicating spontaneous supersymmetry breaking, is a major advancement in our understanding of this theory.

The authors' conjectures on new infrared fermion-fermion dualities involving SU, SO, and Sp gauge theories, as well as their suggested phase diagram for SO/Sp gauge theories with a fermion in the traceless symmetric/antisymmetric tensor representation, provide valuable insights for future research.

Lastly, the authors' conjecture on the value of the time-reversal anomaly for U(n)_n,2n, SO(n)_n, and Sp(n)_n Chern-Simons theories is a significant contribution that can guide future experimental studies.

Overall, this paper presents valuable findings that contribute to our understanding of adjoint QCD in 2+1 dimensions and opens up new directions for further research. Thank you for sharing this fascinating work with the scientific community.
 

What is the purpose of studying the phases of Adjoint QCD3 and dualities?

The study of the phases of Adjoint QCD3 and dualities is important for understanding the behavior of quantum chromodynamics (QCD), which is a fundamental theory of strong interactions in particle physics. It can also shed light on the properties of matter at high temperatures and densities, such as in the early universe or in neutron stars.

What are the different phases of Adjoint QCD3?

The phases of Adjoint QCD3 depend on the temperature and the number of flavors of quarks present in the system. The three main phases are the vacuum phase, the confined phase, and the deconfined phase. In the vacuum phase, quarks are confined and cannot exist freely. In the confined phase, quarks are still confined but can form bound states. In the deconfined phase, quarks can exist freely as individual particles.

What are the dualities in Adjoint QCD3?

Dualities refer to the equivalence between different theories that describe the same physical system. In Adjoint QCD3, there are several dualities that relate the theory to itself at different values of the parameters, such as temperature or number of flavors. These dualities provide different perspectives and insights into the same system.

How do dualities in Adjoint QCD3 relate to other areas of physics?

Dualities in Adjoint QCD3 have connections to other areas of physics, such as string theory and condensed matter physics. For example, some of the dualities in Adjoint QCD3 have analogies in string theory, where they can be used to study black holes and other phenomena. In condensed matter physics, some of the dualities can be applied to systems of fermions, leading to new insights and predictions.

What are the implications of the phases and dualities in Adjoint QCD3 for experimental studies?

The phases and dualities in Adjoint QCD3 can have important implications for experimental studies of QCD, both in the laboratory and in astrophysical observations. For example, the deconfined phase can be probed through experiments with high-energy particle accelerators, while the confined phase can be studied through the properties of hadrons. Additionally, the dualities can provide guidance for the design of experiments and the interpretation of results.

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