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J/psi particle

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J/psi particle
NameJ/psi particle
Other namesJ/ψ, psi, charmonium ground state
Compositioncharm quark and charm antiquark
TypeMeson
GroupHeavy quarkonium
Mass3.0969 GeV/c²
Charge0 e
Parity−1
DiscoverersBurton Richter; Samuel C. C. Ting
Year1974

J/psi particle is a neutral meson consisting of a charm quark bound to a charm antiquark, forming the ground state of the charmonium family. It was contemporaneously discovered in 1974 and precipitated wide revisions in theoretical models by providing clear evidence for the charm quark and validating aspects of quantum chromodynamics. The particle's relatively narrow width, distinctive mass near 3.1 GeV/c², and rich decay spectrum have made it a central probe in experiments at major laboratories and a benchmark in precision tests of the Standard Model.

Discovery

The discovery of the particle occurred independently by two groups: one led by Samuel C. C. Ting at the Brookhaven National Laboratory using the Alternating Gradient Synchrotron and the other by Burton Richter at the Stanford Linear Accelerator Center during experiments with the Stanford Positron Electron Asymmetric Ring. Announced in November 1974, the simultaneous reports produced what is known as the "November Revolution", reshaping research at institutions such as CERN, Fermilab, and DESY. The work of Ting and Richter led to the Nobel Prize in Physics in 1976 and stimulated follow-up programs at the SLAC National Accelerator Laboratory and the Frascati National Laboratory.

Properties

The particle is a vector meson with spin-parity J^P = 1^− and zero electric charge. Its mass, approximately 3.0969 GeV/c², sits below open-charm thresholds and yields a narrow natural width (~93 keV), which contrasts with broader resonances observed at higher energies. As the ground state of the charmonium spectrum, it is described in potential models such as the Cornell potential and in lattice Quantum chromodynamics calculations used at Brookhaven National Laboratory, CERN, and Fermilab. Spectroscopic classification relates it to excited states like the ψ(2S) and χ_c family, and its properties inform effective field theories including nonrelativistic Quantum chromodynamics and potential nonrelativistic Quantum chromodynamics (pNRQCD) used by groups at MIT and Caltech.

Production and detection

Production of the particle occurs in e^+e^− annihilation at colliders like SLAC, KEK, and BEPCII, in hadronic collisions at CERN experiments such as ATLAS and CMS, and in fixed-target experiments at Fermilab. It is produced directly through resonance formation and indirectly via feed-down from higher charmonium states and from B meson decays measured by the Belle and BaBar collaborations. Detection strategies exploit its dileptonic decay channels into e^+e^− and μ^+μ^−, used in detectors including CLEO, LHCb, and ALICE, where precise tracking systems, electromagnetic calorimeters, and muon spectrometers identify the leptons and reconstruct invariant-mass peaks. Triggering and vertexing techniques developed at RHIC and CDF have been instrumental in isolating signals from backgrounds in heavy-ion and proton–proton environments.

Decay modes and branching fractions

Principal detectable decays include leptonic modes (e^+e^−, μ^+μ^−) with sizable branching fractions that facilitate clean spectroscopy at SLAC and KEK. Hadronic decays proceed via annihilation to gluons, producing multihadron final states studied at CERN and Fermilab. Radiative transitions to lower charmonium states (e.g., χ_c → J/ψ γ) and cascade decays from ψ(2S) contribute to observed yields in experiments at Belle II and BESIII. Precision measurements of branching fractions by collaborations at CLEO, BaBar, and LHCb constrain predictions from perturbative Quantum chromodynamics and from models of quarkonium annihilation. Rare and forbidden decays are searched for in flavor-physics programs at Belle, BaBar, and LHCb as probes of physics beyond the Standard Model.

Role in particle physics and theoretical significance

The discovery provided decisive confirmation of the charm quark postulated in the context of the GIM mechanism and influenced the acceptance of the Standard Model. The particle serves as a testing ground for nonperturbative techniques in Quantum chromodynamics, including lattice computations performed at CERN-affiliated collaborations and continuum approaches developed at Princeton University and Harvard University. Measurements of production cross sections, polarization, and medium modifications in heavy-ion collisions at RHIC and LHC inform understanding of quark–gluon plasma formation studied at Brookhaven National Laboratory. The J/psi plays a central role in searches for exotic states such as tetraquarks and hybrid mesons reported by groups at LHCb, Belle, and BESIII, and in precision determinations of charm-quark mass and strong-coupling constant α_s used in global analyses by teams at CERN and PDG.

Category:Mesons