Remnant magnetic fields induce collective rotation in QCD matter via the Einstein-de Haas effect at levels comparable to typical fluid vorticity in heavy-ion collisions.
Navaset al.[Particle Data Group], Phys
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Charm and bottom quark masses are extracted as 1275.8 ± 0.4 MeV and 4177.0 ± 7.2 MeV using PMC-improved conformal series from quarkonium sum-rule moments, agreeing with PDG averages within 1σ.
Node-induced cancellations in the relativistic decay amplitude suppress the D D-bar width of ψ(4040) while leaving D D* and D_s D_s-bar channels sizable.
No signals found for X(3872) to K_S^0 K^± π^∓ or K*(892) K-bar; upper limits on branching fractions relative to π+π- J/ψ are <0.07 and <0.10 at 90% CL.
citing papers explorer
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Einstein-de Haas effect and induced rotation in QCD matter
Remnant magnetic fields induce collective rotation in QCD matter via the Einstein-de Haas effect at levels comparable to typical fluid vorticity in heavy-ion collisions.
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New Determinations of the Charm and Bottom Quark Masses Using QCD Quarkonium Sum Rules
Charm and bottom quark masses are extracted as 1275.8 ± 0.4 MeV and 4177.0 ± 7.2 MeV using PMC-improved conformal series from quarkonium sum-rule moments, agreeing with PDG averages within 1σ.
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Nodal mechanism for the suppressed $D\bar D$ decay of $\psi(4040)$ in the Bethe--Salpeter framework
Node-induced cancellations in the relativistic decay amplitude suppress the D D-bar width of ψ(4040) while leaving D D* and D_s D_s-bar channels sizable.
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Search for the decays $X(3872)\to K_{S}^{0}K^{\pm}\pi^{\mp}$ and $K^*(892)\bar{K}$ at BESIII
No signals found for X(3872) to K_S^0 K^± π^∓ or K*(892) K-bar; upper limits on branching fractions relative to π+π- J/ψ are <0.07 and <0.10 at 90% CL.