Quarkonium Phenomenology in Vacuum

Denis Parganlija

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Quarkonium Phenomenology in Vacuum

Denis Parganlija

High Energy Physics - Phenomenology · Submitted 1 Aug 2012

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

The authors' main claim Contrarily to the naive expectation, the mentioned states are found in the region above 1 GeV.

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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-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 4,912 input tokens, $0.0002 reported.

What the abstract itself states, as probabilities: claims first 0.03 · states limitation 0.09 · human participants 0.01 · controlled comparison 0.05 · randomized assignment 0.01 · states quantitative result 0.77 · compares with prior results 0.38 · mentions code or data availability 0.02.

The abstract, sentence by sentence

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

Broad meson phenomenology in vacuum is discussed in a single model containing scalar, pseudoscalar, vector and axial-vector states both in the non-strange and strange sectors. Emphasis is given to search for quark-antiquark (quarkonium) states in the scalar and axial-vector channels. In particular, the work examines the question whether the scalar quark-antiquark states are found in the energy region below or above 1 GeV in the physical spectrum. Contrarily to the naive expectation, the mentioned states are found in the region above 1 GeV. Additionally, the axial-vector isotriplet state $a_1(1260)$ is described as a quarkonium. These results have consequences for the building of order parameters for the chiral-symmetry breaking of Quantum Chromodynamics (QCD).

background contribution method result interpretation main claim

What the classifier reports for each sentence. The number is the probability it gave the label.
#	sentence	role	the authors' own work	states the main conclusion	strength
s0	Broad meson phenomenology in vacuum is discussed in a single model containing scalar, pseudoscalar, vector and axial-vector states both in the non-strange and strange sectors.	contribution 0.77	0.54	0.05	asserted 0.98
s1	Emphasis is given to search for quark-antiquark (quarkonium) states in the scalar and axial-vector channels.	contribution 0.97	0.45	0.06	asserted 0.75
s2	In particular, the work examines the question whether the scalar quark-antiquark states are found in the energy region below or above 1 GeV in the physical spectrum.	contribution 0.78	0.48	0.06	unclear 0.71
s3	Contrarily to the naive expectation, the mentioned states are found in the region above 1 GeV.	result 1.00	0.85	0.56	asserted 1.00
s4	Additionally, the axial-vector isotriplet state $a_1(1260)$ is described as a quarkonium.	result 0.99	0.77	0.12	asserted 1.00
s5	These results have consequences for the building of order parameters for the chiral-symmetry breaking of Quantum Chromodynamics (QCD).	interpretation 1.00	0.39	0.15	asserted 0.96

What kind of paper the classifier reports this is: theoretical result 0.97 · evidence from argument 0.67.

What was examined, and what was not

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arXiv listing abstract v1

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full text
figures and tables
references and citing sentences
relations to other papers

levels run

P abstract

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S sections
T body sentences
C citations
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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

Broad meson phenomenology in vacuum is discussed in a single model containing scalar, pseudoscalar, vector and axial-vector states both in the non-strange and strange sectors. Emphasis is given to search for quark-antiquark (quarkonium) states in the scalar and axial-vector channels. In particular, the work examines the question whether the scalar quark-antiquark states are found in the energy region below or above 1 GeV in the physical spectrum. Contrarily to the naive expectation, the mentioned states are found in the region above 1 GeV. Additionally, the axial-vector isotriplet state $a_1(1260)$ is described as a quarkonium. These results have consequences for the building of order parameters for the chiral-symmetry breaking of Quantum Chromodynamics (QCD).

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References

Forward citations

Cited by 3 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

Meson vacuum phenomenology in a three-flavor linear sigma model with (axial-)vector mesons
hep-ph 2012-08 conditional novelty 6.0 of 10

A global fit of a three-flavor linear sigma model to meson masses and decays favors scalar quark-antiquark states above 1 GeV, assigning a0(1450) and K*0(1430) as the light scalar quarkonia.
Glueball Decay Rates in the Witten-Sakai-Sugimoto Model
hep-ph 2015-01 conditional novelty 5.0 of 10

In the Witten-Sakai-Sugimoto model the predominantly dilatonic scalar mode at 1487 MeV has decay rates compatible with a glueball component of f0(1500) or f0(1710), while the lighter exotic mode is far too broad.
Decay of the pseudoscalar glueball into scalar and pseudoscalar mesons
hep-ph 2012-08 conditional novelty 5.0 of 10

A single-operator chiral Lagrangian predicts that a pseudoscalar glueball near 2.6 GeV decays dominantly to K K-bar pi, with the three-pion channel forbidden.

How the literature uses it

16 arXiv papers cite this in 61 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 · 48 sentences without a confident label

Builds on it 1 paper

In this section we extend the eLSM [ref] to the four-flavor case.

Phenomenology of charmed mesons in the extended Linear Sigma Model · The Lagrangian of the eLSM for $N_f=4$ · 1.00

Uses its method or tool 2 papers

Hierzu wurden durch das sogenannte “erweiterte Lineare Sigma Modell” (eLSM) [ref] inspirierte effektive Theorien mit derivativen Kopplungen eingesetzt, um den eingangs erwähnten Isovektor $a_0(980)$ und das Isodoublet $K_0^∗(800)$ (auch $κ$ genannt) zu beschreiben.

Dynamical generation of hadronic resonances in effective models with derivative interactions · Deutsche Zusammenfassung · 0.81
We then observe that mixing terms containing axial-vectors and pseudoscalars and $K^⋆$ and $K_0^⋆$ arise in the Lagrangian; these are removed as described in Refs. [ref] .

Phenomenology of Axial-Vector Mesons from an Extended Linear Sigma Model · The Model · 0.93

Uses its data or values 4 papers

The experimental results for the decay width into two pions are Γ^(ex)(f_0(1500)→ππ)/(1505MeV)=0.025(3), Γ^(ex)(f_0(1710)→ππ)/(1722MeV)= {0.017(4) 0.009(2) . where the first result is taken from Ref. , the second from Ref. [ref] using data from the BES collaboration [ref] (upper entry) and the WA102 collaboration [ref] (lower entry), respectively.

Glueball Decay Rates in the Witten-Sakai-Sugimoto Model · Glueball decay to two pions · 0.99
Experimental data imply $Γ_f_0(1500) →ππ/M_f_0(1500) = 0.025 ±0.003$ [ref] and $Γ_f_0(1710) →ππ/M_f_0(1710) ≃0.009$ – $0.017$ [ref] .

Scalar Glueball in a Top-Down Holographic Approach to QCD · The Model and Its Implications · 0.99
The final values for the resonance above $1$ GeV have been given as $m_K_0^∗=1.450±0.001$ GeV and $Γ=0.285±0.012$ GeV [ref] .

Dynamical generation of hadronic resonances in effective models with derivative interactions · Some words on the scalar isodoublet resonances · 0.99

Compares with it 1 paper

Furthermore, the branching ratios of the eLSM are [ref] [equation] which differ from ours, see Eq. ([ref]).

Dynamical generation of hadronic resonances in effective models with derivative interactions · Comparison to the eLSM · 0.91

Cites it as background 3 papers

Detailed calculations of all formulas used in this paper as well as further discussion are presented in Ref. [ref] .

Meson vacuum phenomenology in a three-flavor linear sigma model with (axial-)vector mesons · INTRODUCTION · 0.80
A possible identification of the scalar states in the context of the eLSM was put forward in Refs. [ref] .

Dynamical generation of hadronic resonances in effective models with derivative interactions · Some words on the scalar–isovector resonances · 0.81
We work with a mesonic linear sigma model [ref] as an effective implementation of the strong interaction, which, besides scalar and pseudoscalar mesons, also includes vector and axial-vector mesons [ref] : the so-called eLSM [ref] .

Functional Renormalization Group Study of the Chiral Phase Transition Including Vector and Axial-vector Mesons · Extended Linear Sigma Model · 0.88

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