Radiative decays of the neutral Z(c)(3900)
暂无分享,去创建一个
[1] Li-Yu Daisy Liu,et al. Observation of Z_{c}(3900)^{0} in e^{+}e^{-}→π^{0}π^{0}J/ψ. , 2015, Physical review letters.
[2] E. Swanson. Z b and Z c exotic states as coupled channel cusps , 2014, 1409.3291.
[3] A. S. Nunes,et al. Search for exclusive photoproduction of Z(c)(+/-) (3900) at COMPASS , 2014, 1407.6186.
[4] T. Gutsche,et al. Radiative and dilepton decays of the hadronic molecule Z c + ( 3900 ) , 2014, 1410.0259.
[5] A. Guerrieri,et al. Probing the nature of Z c (′) states via the η c ρ decay , 2014, 1409.3551.
[6] Gang Li,et al. More hidden heavy quarkonium molecules and their discovery decay modes , 2014, 1409.0754.
[7] J. Ping,et al. Interpreting $Z_c(3900)$ and $Z_c(4025)/Z_c(4020)$ as charged tetraquark states , 2014, 1402.0777.
[8] J. M. Dias,et al. Prediction of an $I=1$ $D \bar D^*$ state and relationship to the claimed $Z_c(3900)$, $Z_c(3885)$ , 2014, 1401.8216.
[9] T. Gutsche,et al. Selected strong decay modes of Y(4260) , 2013, 1310.4373.
[10] T. Huang,et al. Analysis of the X(3872), Z c (3900), and Z c (3885) as axial-vector tetraquark states with QCD sum rules , 2013, 1310.2422.
[11] X. Liu 刘,et al. Interpretation of Zb(10610) and Zb(10650) in the ISPE mechanism and the Charmonium Counterpart , 2012, 1208.2411.
[12] T. Huang,et al. Possible assignments of the X ( 3872 ) , Z c ( 3900 ) and Z b ( 10610 ) as axial-vector molecular states , 2014 .
[13] H. Ke,et al. Is Zc(3900) a molecular state? , 2013, 1307.2414.
[14] T. Gutsche,et al. Strong decays of molecular states Z(c)(+) and Z(c)'(+) , 2013, 1306.0824.
[15] J. M. Dias,et al. $Z^+_c$(3900) decay width in QCD sum rules , 2013, 1304.6433.
[16] Jae Hyun Kim,et al. Study of e+ e- → π+ π- J/ψ and observation of a charged charmoniumlike state at Belle. , 2013, Physical review letters.
[17] Li-Yu Daisy Liu,et al. ec 2013 Observation of a charged charmoniumlike structure Z c (4020) and search for the Z c (3900) in e + e − → π + π − h c , 2013 .
[18] T. Gutsche,et al. Decays of Z(b)(+) and Z(b)'(+) as hadronic molecules , 2012, 1203.1894.
[19] Wei Wang,et al. Tetraquark Interpretation of the Charged Bottomonium-like states $Z_b^{+-}(10610)$ and $Z_b^{+-}(10650)$ and Implications , 2011, 1110.1333.
[20] Xiang Liu,et al. Predicted charged charmoniumlike structures in the hidden-charm dipion decay of higher charmonia , 2011, 1106.5290.
[21] Xiang Liu,et al. Z b ( 10 610 ) and Z b ( 10 650 ) structures produced by the initial single pion emission in the Υ ( 5 S ) decays , 2011, 1106.3798.
[22] Xiang Liu,et al. Long-distant contribution and χc1 radiative decays to light vector meson , 2010, 1005.0066.
[23] T. Gutsche,et al. X(3872) as a hadronic molecule and its decays to charmonium states and pions , 2009, 0903.5416.
[24] T. Gutsche,et al. New heavy mesons as hadronic molecules , 2008 .
[25] T. Gutsche,et al. Strong and radiative decays of the D(s0)*(2317) meson in the DK-molecule picture , 2007, 0705.0254.
[26] A. Polosa,et al. Diquark-antidiquarks with hidden or open charm and the nature of X(3872) , 2004, hep-ph/0412098.
[27] F. Fazio,et al. B−→K−χc0 decay from charmed meson rescattering , 2002, hep-ph/0207061.
[28] S. H. Lee,et al. J/ψ absorption by π and ρ mesons in a meson exchange model with anomalous parity interactions , 2000, nucl-th/0010064.
[29] G. Nardulli,et al. Phenomenology of heavy meson chiral lagrangians , 1996, hep-ph/9605342.
[30] S. Weinberg. Elementary Particle Theory of Composite Particles , 1963 .
[31] A. Salam. Lagrangian theory of composite particles , 1962 .