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ψ(2S)

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Parent: BESIII Hop 5
Expansion Funnel Raw 49 → Dedup 0 → NER 0 → Enqueued 0
1. Extracted49
2. After dedup0 (None)
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ψ(2S)
Nameψ(2S)
Other namespsi(2S), ψ′
Compositioncharm quark and charm antiquark
Parity−1
Mass3686.10 MeV/c^2
Width0.299 MeV
Lifetime6.9×10^−22 s

ψ(2S) is the first radial excitation of the charmonium vector meson family, a bound state of a charm quark and a charm antiquark observed in high-energy experiments. It sits above the mass of the J/ψ and exhibits a rich spectrum of electromagnetic and hadronic transitions that have been probed by collaborations at accelerator facilities worldwide. The resonance has played a central role in testing quantum chromodynamics and in calibrating detectors at colliders.

Discovery and Naming

The resonance was discovered during the period of intense particle spectroscopy investigations that followed the simultaneous observations of the J/ψ by teams at SLAC and Brookhaven National Laboratory and is associated historically with groups working at Cornell University and CERN. Early experimental signals were obtained in e+e− annihilation studies at storage rings such as ADONE and in fixed-target experiments at Fermilab. The naming convention ψ(2S) reflects the spectroscopic notation used by the Particle Data Group and by theorists who adopted quantum numbers from the quark model; the label distinguishes the radial excitation from the ground-state vector meson J/ψ and from higher orbital excitations studied at DESY and KEK. Key collaborations including BESIII, CLEO, BaBar, and Belle contributed to precision determinations of its mass and width during decades of spectroscopy.

Properties and Decay Modes

The particle has quantum numbers J^PC = 1^−− and a mass measured at high precision by experiments such as BESIII and CLEO-c, with electromagnetic and strong decay channels catalogued by the Particle Data Group. Prominent decays include radiative transitions to lower charmonium states observed in detectors at SLAC PEP-II and KEK-B, hadronic transitions involving pion emission measured by Belle II and BaBar, and dileptonic decays (e+e−, μ+μ−) used as calibration channels by LHC experiments such as ATLAS and CMS. Hadronic annihilation into light hadrons proceeds via intermediate gluon states described in perturbative calculations used by theorists at institutions including Princeton University and MIT. The total decay width and branching fractions have been refined by analyses from LHCb and by joint efforts at IHEP and INR.

Production Mechanisms and Experimental Measurements

Production of the resonance occurs in e+e− annihilation at storage rings like BEPCII and via initial-state radiation at asymmetric factories such as PEP-II and KEKB. It is produced in hadronic collisions at CERN SPS and Fermilab Tevatron and studied in proton–proton interactions at LHC experiments including LHCb and ALICE. Secondary production channels include B-meson decays examined by Belle and BaBar, and charmonium feed-down measured by heavy-ion programs at RHIC and LHC heavy-ion runs. Precision cross-section measurements have been reported in publications from IHEP Beijing and collaborative analyses involving JINR and TRIUMF. Detector technologies from SLAC silicon trackers to CERN calorimeters and muon systems at CMS and ATLAS have been crucial for separating ψ(2S) signals from backgrounds like Drell–Yan and open-charm production studied at FNAL.

Theoretical Interpretations and Quark Model Context

In the context of the constituent quark model and potential models developed by theorists at Cornell University and Yale University, ψ(2S) is interpreted as the 2S radial excitation of the c c̄ system; lattice QCD calculations performed by collaborations at CERN and Brookhaven National Laboratory provide nonperturbative input to its spectrum. Radiative transitions are modeled with effective field theory approaches from groups at Harvard University and University of California, Berkeley, while perturbative QCD corrections and nonrelativistic QCD (NRQCD) factorization methods have been advanced by researchers at Caltech and Institute for Advanced Study. The resonance has been used to probe color-octet mechanisms discussed in seminars at SLAC and to test potential models developed by Eichten and colleagues. Comparisons with bottomonium excitations studied at KEK and LHCb help constrain heavy-quark spin symmetry and relativistic corrections analyzed by theorists at Perimeter Institute and University of Cambridge.

Role in Particle Physics Experiments and Applications

ψ(2S) has served as an experimental benchmark for detector calibration across experiments at CERN, SLAC, and KEK, providing clean dilepton signals for momentum scale and alignment studies used by collaborations such as ATLAS, CMS, and LHCb. Its production and suppression patterns in heavy-ion programs at RHIC and CERN are studied alongside quark-gluon plasma signatures investigated by ALICE and inform theoretical models developed at Brookhaven National Laboratory. Measurements of branching fractions by BESIII contribute to precision tests of electroweak and strong interaction phenomenology pursued at Institute of High Energy Physics (IHEP) and influence global fits coordinated with the Particle Data Group and analysis groups at SLAC. The resonance also features in educational outreach and museum exhibits at institutions like CERN and Fermilab where its discovery history and role in confirming the charm quark hypothesis are presented.

Category:Charmonium