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Holonomy potential and confinement from a simple model of the gauge topology
High Energy Physics - Phenomenology · Submitted 3 May 2013
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Using a simple model with excluded volume and lattice data on caloron density we find that repulsive part of the potential is robust enough to induce the phase transition at the right temperature.
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The abstract, sentence by sentence
We discuss an ensemble of topological solitons -- instanton-dyons and antidyons - in SU(2) pure gauge theory at finite temperatures above and below the deconfinement phase transition temperature. The main focus is on the combined effect of this ensemble on the so called effective holonomy potential, which drives the confinement/deconfinement phase transition. Using a simple model with excluded volume and lattice data on caloron density we find that repulsive part of the potential is robust enough to induce the phase transition at the right temperature. Model's predictions -- the holonomy potential, electric and magnetic screening masses as a function of T -- are in qualitative agreement with the available lattice data. Further predictions are densities of various dyon types as a function of temperature: while some lattice measurements of them had been made, much more accurate data are needed to test these predictions.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We discuss an ensemble of topological solitons -- instanton-dyons and antidyons - in SU(2) pure gauge theory at finite temperatures above and below the deconfinement phase transition temperature. | background 0.55 | 0.31 | 0.03 | asserted 0.80 |
| s1 | The main focus is on the combined effect of this ensemble on the so called effective holonomy potential, which drives the confinement/deconfinement phase transition. | contribution 0.94 | 0.37 | 0.10 | asserted 0.88 |
| s2 | Using a simple model with excluded volume and lattice data on caloron density we find that repulsive part of the potential is robust enough to induce the phase transition at the right temperature. | result 0.96 | 0.95 | 0.70 | asserted 0.99 |
| s3 | Model's predictions -- the holonomy potential, electric and magnetic screening masses as a function of T -- are in qualitative agreement with the available lattice data. | result 0.98 | 0.79 | 0.17 | asserted 0.76 |
| s4 | Further predictions are densities of various dyon types as a function of temperature: while some lattice measurements of them had been made, much more accurate data are needed to test these predictions. | future work 0.76 | 0.62 | 0.04 | asserted 0.70 |
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The paper
Original abstract
We discuss an ensemble of topological solitons -- instanton-dyons and antidyons - in SU(2) pure gauge theory at finite temperatures above and below the deconfinement phase transition temperature. The main focus is on the combined effect of this ensemble on the so called effective holonomy potential, which drives the confinement/deconfinement phase transition. Using a simple model with excluded volume and lattice data on caloron density we find that repulsive part of the potential is robust enough to induce the phase transition at the right temperature. Model's predictions -- the holonomy potential, electric and magnetic screening masses as a function of T -- are in qualitative agreement with the available lattice data. Further predictions are densities of various dyon types as a function of temperature: while some lattice measurements of them had been made, much more accurate data are needed to test these predictions.
Human review
References
How the literature uses it
20 arXiv papers cite this in 31 sentences
Papers citing it · 22 sentences without a confident label
Uses its method or tool 1 paper
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Therefore, we follow [ref] and represent the grand partition function for the ensemble as follows
Dynamical de Sitter phase and nontrivial holonomy in strongly coupled gauge theories in expanding Universe · The grand canonical ensemble of monopoles with nontrivial holonomy ([ref]) · 0.93
Uses its data or values 1 paper
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The fit shown in Fig.1 of Ref. [ref] corresponds to non-interacting gas of calorons, and it give Λ_calorons = 0.36 T_c where $T_c$ is the deconfinement transition temperature, defined in the same lattice work.
Interacting Ensemble of the Instanton-dyons and Deconfinement Phase Transition in the SU(2) Gauge Theory · Units and holonomy · 1.00
Compares with it 1 paper
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M:e^-b-iσ L:e^b+iσ M̅: e^-b+iσ L̅ :e^b-iσ Note that these assignments are consistent with those suggested in [ref] using different arguments.
Light Quarks in the Screened Dyon-Anti-Dyon Coulomb Liquid Model II · Bosonic fields · 0.80
Cites it as background 6 papers
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We review the relevant results from refs [ref] on this matter below in section [ref].
Dynamical de Sitter phase and nontrivial holonomy in strongly coupled gauge theories in expanding Universe · Nontrivial holonomy ([ref]) in Euclidean space. Few technical details. · 0.98
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A very simple model of a de-confinement transition has been proposed by Shuryak and Sulejmanpasic [ref] through the use of dyon-antidyon “repulsive cores".
Light Quarks in the Screened Dyon-Anti-Dyon Coulomb Liquid Model II · Introduction · 0.96
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For related works, see [ref] .
New Methods in QFT and QCD: From Large-N Orbifold Equivalence to Bions and Resurgence · Calculability and the Deconfinement Phase Transition · 0.94
What it cites · 12 sentences without a confident label
Uses data or values from 1 paper
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For definiteness, we start with fixing global parameters of the $SU(2)$ gauge theory topology, using lattice works [ref] and [ref] .
The dyonic picture of topological objects in the deconfined phase · Introduction · 0.89
Compares with 1 paper
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To conclude this section, let us mention that the potentials [ref] and [ref] are similar to the one discussed in [ref] for the case of pure Yang-Mills.
Continuity, Deconfinement, and (Super) Yang-Mills Theory · The holonomy potential · 0.93
Cites as background 7 papers
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At nonzero asymptotic holonomy $A_0(r→∞)0$ the instanton solution is modified and as a result the instanton is split into $N_c$ constituents known as KvBLL self-dual instanton-dyons [ref] .
Monopoles and Instantons on Partially Compactified D-Branes · Introduction · 0.93
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At nonzero asymptotic holonomy $A_0(r→∞)0$ the instanton solution is modified and as a result the instanton is split into $N_c$ constituents known as KvBLL self-dual instanton-dyons [ref] .
Monopole Constituents inside SU(n) Calorons · Introduction · 0.93
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Interactions and statistical ensemble of instanton-dyons and antidyons have been studied qualitatively using neutral dyon-antidyon pairs in [ref] , recently complemented by first numerical simulations [ref] .
The Chiral Symmetry Breaking/Restoration in Dyonic Vacuum · Introduction · 0.89
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