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Non-Perturbative Yang-Mills Condensate as Dark Energy

General Relativity and Quantum Cosmology · Submitted 19 Sep 2015

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim Using non-perturbative techniques mutated from the functional renormalization group procedure, we finally show that the minimum in $\theta$ of the effective Lagrangian exists, thus YMC can actually take place.

how it is stated · asserted 1.00 read the record →

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arXiv ID1509.05824 (version 1)
Pith IDR3P6WULN, Pith's permanent record of this paper and its review
CitationAntonino Marcian\`o, Claudia Antolini, Pietro Don\`a, Yang Zhang. "Non-Perturbative Yang-Mills Condensate as Dark Energy." arXiv:1509.05824 (2015). https://pith.science/paper/R3P6WULN
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Compiled by classifier-1.13.0 via TypeSafe API, question bank abstract-p1-20260923, 2026-09-23: 1 request, 7,185 input tokens.

What the abstract itself states, as probabilities: claims first 0.05 · states limitation 0.51 · human participants 0.01 · controlled comparison 0.07 · randomized assignment 0.01 · states quantitative result 0.86 · compares with prior results 0.93 · mentions code or data availability 0.01.

The abstract, sentence by sentence

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

Models based on Yang-Mills condensate (YMC) have been advocated in the literature and claimed to be successful candidates to explain dark energy. Several instantiations of this simple idea have been considered, the most promising of which are reviewed here. Nevertheless, results previously attained heavily relied on the perturbative approach to the analysis of the effective Yang-Mills action, which is only adequate in the asymptotically-free limit, and were extended into a regime, the infrared limit, in which confinement is expected. We show that if a minimum of the effective Lagrangian in $\theta \!=\! - F_{\, \, \mu \nu}^a \, F^{a \mu \nu}/2$ exists, a YMC forms that drives the Universe toward an accelerated de Sitter phase. The details of the models depend weakly on the specific form of the effective Yang-Mills Lagrangian. Using non-perturbative techniques mutated from the functional renormalization group procedure, we finally show that the minimum in $\theta$ of the effective Lagrangian exists, thus YMC can actually take place. The non-perturbative model has properties similar to the ones of the perturbative model. In the early stage of the universe, the YMC equation of state has an evolution that resembles the radiation component, i.e. $w_y \rightarrow 1/3$. However, in the late stage, $w_y$ naturally runs to the critical state with $w_y =-1$, and the universe transits from matter-dominated into dark energy dominated stage only recently, at a redshift the value of which depends on the initial conditions that are chosen while solving the dynamical system.

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 Models based on Yang-Mills condensate (YMC) have been advocated in the literature and claimed to be successful candidates to explain dark energy. background 1.00 0.03 0.03 asserted 0.54
s1 Several instantiations of this simple idea have been considered, the most promising of which are reviewed here. background 0.94 0.23 0.02 asserted 0.83
s2 Nevertheless, results previously attained heavily relied on the perturbative approach to the analysis of the effective Yang-Mills action, which is only adequate in the asymptotically-free limit, and were extended into a regime, the infrared limit, in which confinement is expected. gap 0.77 0.06 0.03 asserted 0.98
s3 We show that if a minimum of the effective Lagrangian in $\theta \!=\! - F_{\, \, \mu \nu}^a \, F^{a \mu \nu}/2$ exists, a YMC forms that drives the Universe toward an accelerated de Sitter phase. result 0.83 0.77 0.36 asserted 0.86
s4 The details of the models depend weakly on the specific form of the effective Yang-Mills Lagrangian. result 0.75 0.35 0.04 asserted 0.99
s5 Using non-perturbative techniques mutated from the functional renormalization group procedure, we finally show that the minimum in $\theta$ of the effective Lagrangian exists, thus YMC can actually take place. result 0.55 0.96 0.52 asserted 1.00
s6 The non-perturbative model has properties similar to the ones of the perturbative model. result 0.82 0.69 0.09 asserted 1.00
s7 In the early stage of the universe, the YMC equation of state has an evolution that resembles the radiation component, i.e. $w_y \rightarrow 1/3$. result 1.00 0.80 0.06 asserted 0.98
s8 However, in the late stage, $w_y$ naturally runs to the critical state with $w_y =-1$, and the universe transits from matter-dominated into dark energy dominated stage only recently, at a redshift the value of which depends on the initial conditions that are chosen while solving the dynamical system. result 0.95 0.82 0.20 asserted 1.00

What kind of paper the classifier reports this is: theoretical result 0.99 · evidence from proof or derivation 0.73.

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  • references and citing sentences
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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

Models based on Yang-Mills condensate (YMC) have been advocated in the literature and claimed to be successful candidates to explain dark energy. Several instantiations of this simple idea have been considered, the most promising of which are reviewed here. Nevertheless, results previously attained heavily relied on the perturbative approach to the analysis of the effective Yang-Mills action, which is only adequate in the asymptotically-free limit, and were extended into a regime, the infrared limit, in which confinement is expected. We show that if a minimum of the effective Lagrangian in $\theta \!=\! - F_{\, \, \mu \nu}^a \, F^{a \mu \nu}/2$ exists, a YMC forms that drives the Universe toward an accelerated de Sitter phase. The details of the models depend weakly on the specific form of the effective Yang-Mills Lagrangian. Using non-perturbative techniques mutated from the functional renormalization group procedure, we finally show that the minimum in $\theta$ of the effective Lagrangian exists, thus YMC can actually take place. The non-perturbative model has properties similar to the ones of the perturbative model. In the early stage of the universe, the YMC equation of state has an evolution that resembles the radiation component, i.e. $w_y \rightarrow 1/3$. However, in the late stage, $w_y$ naturally runs to the critical state with $w_y =-1$, and the universe transits from matter-dominated into dark energy dominated stage only recently, at a redshift the value of which depends on the initial conditions that are chosen while solving the dynamical system.

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How the literature uses it

9 arXiv papers cite this in 17 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 · 11 sentences without a confident label

Contests it 1 paper
  • An alternative model to our approach has been recently suggested: the dark energy could be generated by an invisible Yang-Mills or Invisible QCD condensates [ref] In this case, the generation of a neutrino mass gap is similarly possible but it seems ruled out by observations of unconfined neutrinos.

    Born-Infeld condensate as a possible origin of neutrino masses and dark energy · Conclusions and outlooks · contest 0.74

Builds on it 1 paper
  • The effective action of the quantum YM gauge $SU(N)$($N=2,3,…$) theory consistently incorporating the vacuum polarisation effects and leading to the trace anomaly can be properly generalised to the FLRW background as follows [ref] (see also Ref. [ref] ) [equation] where the YM field and the corresponding stress tensor are defined as usual [equation] with internal (in adjoint representation) $a,b,c=1,… N^2-1$ and Lorentz $μ,ν=0,1,2,3$ indices and the gauge coupling $g̅=g̅(J)$ satisfying the RG evolution equation [ref] [equation] Depending on the sign of the invariant $J$, one distinguishes the chromoelectric $J>0$ and chromomagnetic $J<0$ YM fields.

    Mirror QCD and Cosmological Constant · Effective Yang-Mills theory in expanding universe · 0.91

Cites it as background 4 papers

What it cites · 3 sentences without a confident label

Cites as background 5 papers

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