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Glueball QCD Simulator SU(3) Gauge

Flux Tension σ: 0.98 GeV/fm
Two-Gluon Color Singlet (0++)
Drag nodes or click to inject energy
Color/Anti-color Octet Gluons
Chromoelectric Flux Tube
0.65 fm
Cornell Static Potential: V(r) = -4/3 · (αs/r) + σr V(r) = 1.14 GeV
Pair Production Threshold (2mq)

Resonance State Configuration

SU(3) Color Singlet

Coupling & String Parameters

0.36

Controls Coulombic short-range gluon interaction (Asymptotic freedom at low values).

0.98

Energy stored per unit length of chromoelectric flux tube (∼ 14-16 tons of force).

0.45

Thermal/quantum noise driving virtual gluon loop creations in the vacuum.

Lattice QCD Resonance Data

JPC = 0⁺⁺
Pure Gauge Glueball Fraction: 84.2%
Predicted Mass (LQCD)
1710 ± 40 MeV
Decay Width Γ
139 ± 8 MeV
Decay Channels: f₀(1710) → K K̄ (dominant, 65%), ηη (20%), ππ (chiral suppressed 15%)

1. Non-Abelian SU(3) & Self-Interactions

Unlike quantum electrodynamics (QED) photons which carry zero electric charge, quantum chromodynamics (QCD) gluons carry non-zero color charge (8 Gell-Mann generators in SU(3)). Because gluons interact directly with one another via 3-gluon and 4-gluon vertices, they can bind together without valence quarks into composite colorless hadrons called glueballs.

2. Color Confinement & String Breaking

Self-attraction between gluons squeezes the chromoelectric lines into a tight flux tube with constant string tension (σ ≈ 1 GeV/fm ≈ 100,000 N). As separation r increases, potential energy climbs linearly until it exceeds the mass threshold for creating a quark-antiquark (qq̄) pair, breaking the string into conventional mesons.

3. Experimental Hunt: BESIII & X(2370)

Radiative decays of J/ψ particles at colliders (such as the Beijing Spectrometer BESIII) provide a gluon-rich environment. Recent measurements of the resonance X(2370) in J/ψ → γ π⁺π⁻η′ match quenched Lattice QCD predictions for the lightest pseudoscalar glueball (0⁻⁺).