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The Instanton-Dyon Liquid Model V: Twisted Light Quarks
High Energy Physics - Phenomenology · Submitted 9 Jun 2016
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The low temperature phase is center symmetric but breaks spontaneously flavor symmetry with $N_f-1$ massless pions.
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
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The abstract, sentence by sentence
We discuss an extension of the instanton-dyon liquid model that includes twisted light quarks in the fundamental representation with explicit $Z_{N_c}$ symmetry for the case with equal number of colors $N_c$ and flavors $N_f$. We map the model on a 3-dimensional quantum effective theory, and analyze it in the mean-field approximation. The effective potential and the vacuum chiral condensates are made explicit for $N_f=N_c=2, 3$. The low temperature phase is center symmetric but breaks spontaneously flavor symmetry with $N_f-1$ massless pions. The high temperature phase breaks center symmetry but supports finite and unequal quark condensates.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We discuss an extension of the instanton-dyon liquid model that includes twisted light quarks in the fundamental representation with explicit $Z_{N_c}$ symmetry for the case with equal number of colors $N_c$ and flavors $N_f$. | contribution 0.99 | 0.86 | 0.09 | asserted 0.91 |
| s1 | We map the model on a 3-dimensional quantum effective theory, and analyze it in the mean-field approximation. | method 0.98 | 0.93 | 0.04 | asserted 0.96 |
| s2 | The effective potential and the vacuum chiral condensates are made explicit for $N_f=N_c=2, 3$. | contribution 0.68 | 0.93 | 0.09 | asserted 1.00 |
| s3 | The low temperature phase is center symmetric but breaks spontaneously flavor symmetry with $N_f-1$ massless pions. | result 1.00 | 0.88 | 0.29 | asserted 1.00 |
| s4 | The high temperature phase breaks center symmetry but supports finite and unequal quark condensates. | result 1.00 | 0.88 | 0.21 | asserted 1.00 |
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The paper
Original abstract
We discuss an extension of the instanton-dyon liquid model that includes twisted light quarks in the fundamental representation with explicit $Z_{N_c}$ symmetry for the case with equal number of colors $N_c$ and flavors $N_f$. We map the model on a 3-dimensional quantum effective theory, and analyze it in the mean-field approximation. The effective potential and the vacuum chiral condensates are made explicit for $N_f=N_c=2, 3$. The low temperature phase is center symmetric but breaks spontaneously flavor symmetry with $N_f-1$ massless pions. The high temperature phase breaks center symmetry but supports finite and unequal quark condensates.
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References
How the literature uses it
10 arXiv papers cite this in 13 sentences
Papers citing it · 6 sentences without a confident label
Cites it as background 7 papers
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Thermodynamic ensembles of dyons were studied analytically [ref] via mean-field approximation, as well as numerically [ref] .
Towards a semi-classical description of QCD vacuum around $T_c$ · Introduction · 0.88
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In this theory, the Polyakov loop is the true order parameter for center symmetry even fermions appear. $ℤ_3$-QCD is an interesting and instructive theory which is useful for understanding the deconfinement transition of QCD [ref] .
Roberge-Weiss transitions at different center symmetry breaking patterns in a $\mathbb{Z}_{3}$-QCD model · Introduction · 0.97
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We will focus on a series of papers devoted to high-density phase and mean field approximation [ref] in section [ref], and on the direct numerical simulation of the dyon ensembles [ref] in section [ref].
Recent progress in understanding deconfinement and chiral restoration phase transitions · Introduction · 0.86
What it cites · 14 sentences without a confident label
Builds on 1 paper
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This work is a continuation of our earlier studies [ref] of the gauge topology using the instanton-dyon liquid model.
Light Adjoint Quarks in the Instanton-Dyon Liquid Model IV · Introduction · 0.83
Uses the method or tool of 2 papers
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As we noted earlier, we use it to regulate the infrared sensitivity of the ds-contributions in ([ref]) through a suitable redefinition of the fugacities $f_2,3$ as in [ref] .
Light Adjoint Quarks in the Instanton-Dyon Liquid Model IV · $N_c$=$N_f=3$ in general asymmetric phase · 0.87
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Following [ref] the moduli determinants in ([ref]) can be fermionized using $2N_c$ pairs of ghost fields $χ_m,χ^†_m$ for the instanton-dyons and $2N_c$ for the instanton-anti-dyons.
Confining ensemble of dyons · SU($N_c$) ensemble · 0.99
Compares with 2 papers
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A further comparison between the mean field results derived in this paper, with the direct simulations [ref] of the instanton-dyon model and lattice results [ref] , is obviously of great interest.
Lattice study on QCD-like theory with exact center symmetry · Conclusions · 0.84
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A further comparison between the mean field results derived in this paper, with the direct simulations [ref] of the instanton-dyon model and lattice results [ref] , is obviously of great interest.
Instanton-dyon Ensembles III: Exotic Quark Flavors · Conclusions · 0.84
Cites as support 2 papers
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The random hopping of these zero modes in the instanton-dyon liquid is at the origin of the spontaneous breaking of chiral symmetry as has been shown both numerically [ref] and using mean-field methods [ref] .
The Chiral Symmetry Breaking/Restoration in Dyonic Vacuum · Introduction · 0.97
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The random hopping of these zero modes in the instanton-dyon liquid is at the origin of the spontaneous breaking of chiral symmetry as has been shown both numerically [ref] and using mean-field methods [ref] .
QCD Topology at Finite Temperature: Statistical Mechanics of Selfdual Dyons · Introduction · 0.97
Cites as background 7 papers
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The starting point of the model are the KvBLL instantons threaded by finite holonomies and their splitting into instanton-dyon constituents [ref] , with strong semi-classical interactions [ref] .
Confining ensemble of dyons · Introduction · 0.83
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The starting point of the model are the KvBLL instantons threaded by finite holonomies and their splitting into instanton-dyon constituents [ref] , with strong semi-classical interactions [ref] .
Classical interactions of the instanton-dyons with antidyons · Introduction · 0.83
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A numerical analysis in the the instanton-dyon liquid model with $N_f=N_c=2$ was recently presented in [ref] .
Instanton-dyon Ensembles III: Exotic Quark Flavors · Introduction · 0.84
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