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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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arXiv ID1606.02996 (version 1)
Pith IDKCVAPKLC, Pith's permanent record of this paper and its review
CitationEdward Shuryak, Ismail Zahed, Yizhuang Liu. "The Instanton-Dyon Liquid Model V: Twisted Light Quarks." arXiv:1606.02996 (2016). https://pith.science/paper/KCVAPKLC
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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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Compiled by classifier-1.13.0 via TypeSafe API, question bank abstract-p1-20260923, 2026-09-23: 1 request, 4,224 input tokens.

What the abstract itself states, as probabilities: claims first 0.03 · states limitation 0.17 · human participants 0.01 · controlled comparison 0.02 · randomized assignment 0.01 · states quantitative result 0.55 · compares with prior results 0.07 · mentions code or data availability 0.02.

The abstract, sentence by sentence

arXiv listing abstract v1. Results and the main claim are underlined; .

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

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
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

What kind of paper the classifier reports this is: theoretical result 1.00 · evidence from proof or derivation 0.98.

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Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

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

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

Papers citing it · 6 sentences without a confident label

Cites it as background 7 papers

What it cites · 14 sentences without a confident label

Builds on 1 paper
Uses the method or tool of 2 papers
  • 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

  • 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
  • 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

  • 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
Cites as background 7 papers
  • 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

  • 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

  • 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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