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Study of χ_{bJ}(2P)→ωϒ(1S) at Belle
Physical Review Letters
|October 5, 2025
Summary
Researchers observed new evidence for the near-threshold hadronic transition chi_b0(2P) to omegaUpsilon(1S). This finding provides insights into heavy quarkonium physics and challenges predictions from quantum chromodynamics multipole expansion models.
Area of Science:
- Particle Physics
- Quantum Chromodynamics (QCD)
- Hadron Spectroscopy
Background:
- The study investigates hadronic transitions between excited bottomonium states (χ_{bJ}(2P)) and the Upsilon(1S) meson.
- Understanding these transitions is crucial for mapping the spectrum of heavy quarkonium and testing QCD predictions.
- Previous studies have focused on charmonium sector analogs, like the χ_{c1}(3872) decay.
Purpose of the Study:
- To search for and measure the branching fractions of χ_{bJ}(2P)→ωϒ(1S) transitions, where ω decays into three pions.
- To provide the first evidence for the near-threshold transition χ_{b0}(2P)→ωϒ(1S).
- To compare the measured ratios of transition rates with theoretical expectations, particularly from the QCD multipole expansion.
Main Methods:
- Analysis of 28.2×10^6 Υ(3S) mesons collected by the Belle detector.
- Identification of ω mesons via their decay into π^{+}π^{-}π^{0}.
- Statistical analysis to determine branching fractions and their uncertainties.
Main Results:
- First evidence for the near-threshold transition χ_{b0}(2P)→ωϒ(1S) with a branching fraction of (0.55±0.19±0.07)%.
- Measured branching fractions for χ_{b1}(2P)→ωϒ(1S) as (2.39_{-0.19}^{+0.20}±0.24)% and χ_{b2}(2P)→ωϒ(1S) as (0.47_{-0.12}^{+0.13}±0.06)%.
- The measured ratio of J=2 to J=1 transitions deviates by 3.3 standard deviations from QCD multipole expansion predictions.
Conclusions:
- The observation of the χ_{b0}(2P)→ωϒ(1S) transition, analogous to near-threshold charm decays, offers new insights into heavy quarkonium dynamics.
- The measured branching fractions for the P-wave states are confirmed.
- The discrepancy in the transition ratio suggests potential refinements needed in the theoretical framework of the QCD multipole expansion for heavy quarkonium.
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