* fo(98o)rded as mixing of and ssour cnnalationLand forΦ→ foss[fo(980))=cos0|ss)+sin0|nn)r(J/b→ fow)~r(J/b→ fod)nnExperimental dataModeBABARBelleCLEOCDFNew Avg.PDG2006 Avg.9.2+0.89.5 ± 1.0+8.8K+fo(980) t8.9±1.08.8 ±0.8+0.87.6 ± 1.7±0.8K°fo(980) t5.9±0.85.5±0.7±0.65.5±0.7±0.6The earlier studyC.H.Chen,Phys.Rev.D67, 014012(2003)PQCDC.H. Chen, Phys.Rev.D 67, 094011 (2003)QCDF, Cheng et al PRD 71,054020(2005),PRD73, 014017(2006)Generalized factorization +new physics, A.Giri, et al, hep-ph/060808869/17/2026高能物理学会第七届年会@桂林
❖ is regarded as mixing of and in our calculation and : : Experimental data The earlier study ⚫ PQCD ⚫ QCDF, Cheng et al PRD 71,054020(2005), PRD73, 014017(2006) ⚫ Generalized factorization +new physics, A. Giri, et al, hep-ph/0608088. 9/17/2026 高能物理学会第七届年会@桂林 6
fo(13and belassoimed tofbel mioing of qark-antiquark and glueball statesThe mixing scheme is still under controversyCheng et alClose and Zhao0.070.40(fo(1370))(0.91(IM)fo(1370)/0.780.510.36((M))[S)[S)0.84fo(1500)0.410.35fo(1500)0.03-0.540.84一(G))(0.090.930.36(fo(1710))(G))(fo(1710))0.180.930.32The decays lB-→ x(1500)Kneasured in but not in FB _'KkKB(B-→ fo(1500)K-) = (471.9± 51.3) ×10-6, Solution IB(B-→ fo(1500)K-) = (67.1±14.4) ×10-6, Solution II79/17/2026高能物理学会第七届年会@桂林
, and are assumed to be mixing of qarkantiquark and glueball states Cheng et al Close and Zhao The mixing scheme is still under controversy The decays have been measured in but not in B Kpipi 9/17/2026 高能物理学会第七届年会@桂林 7