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- [1] Study of the f2(1270) , f2′(1525) , f0(1370) and f0(1710) in the J/ψ radiative decays The European Physical Journal A, 2010, 44 : 305 - 311
- [3] Study of the f2(1270), f ′2(1525), and (K)over-bar2*(1430), f0(1370) and f0(1710) production from ψ(nS) and Υ(nS) decays PHYSICAL REVIEW D, 2015, 91 (09):
- [4] ψ(nS) and γ(nS) decay into f2(1270), f'2(1525), (K)over-bar2*(1430), f0(1370) and f0(1710) production XVITH INTERNATIONAL CONFERENCE ON HADRON SPECTROSCOPY (HADRON2015), 2016, 1735
- [5] photon and one-photon -one-vector meson decay widths of the f0(1370), f2(1270), f0(1710), f2′(1525), and K2*(1430) PHYSICAL REVIEW D, 2010, 81 (05):
- [6] The f0(1370), f0(1710), f2(1270), f′2(1525), and K*2(1430) as dynamically generated states from vector meson - vector meson interaction INTERNATIONAL WORKSHOP ON CHIRAL SYMMETRY IN HADRONS AND NUCLEI, 2010, 1322 : 214 - +
- [8] The Decays (B)over-bar0 and (B)over-barS0 Into J/ψ and f0(1370), f0(1710), f2(1270), f'2(1525), K2*(1430) and Vector-Vector Molecules XVITH INTERNATIONAL CONFERENCE ON HADRON SPECTROSCOPY (HADRON2015), 2016, 1735
- [9] Hadronic and radiative three-body decays of J/ψ involving the scalars f0(1370), f0(1500), and f0(1710) PHYSICAL REVIEW D, 2011, 84 (03):
- [10] γγ decay of the f0(1370) and f2(1270) resonances in the hidden gauge formalism PHYSICAL REVIEW D, 2009, 79 (11):