Results 81 to 90 of about 382 (185)
Strong decays of vector mesons to pseudoscalar mesons in the relativistic quark model
Physics Letters B, 2015 Strong decays of vector (S13) mesons to the pair of pseudoscalar (S01) mesons are considered in the framework of the microscopic decay mechanism and the relativistic quark model based on the quasipotential approach.
D. Ebert, R.N. Faustov, V.O. Galkin
doaj +1 more source
Direct CP Violation from Isospin Symmetry Breaking Effects for the Decay Process B-s→P(V)π0 in PQCD
Advances in High Energy Physics, 2019 We investigate the direct CP violation for the decay process of B-s→P(V)π0 (P,V refer to the pseudoscalar meson and vector meson, resp.) via isospin symmetry breaking effects from the π0-η-η′ mixing mechanism in PQCD factorization approach.
Gang Lü, Qin-Qin Zhi
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THE TRANSITION OF VIRTUAL PHOTONS INTO PSEUDOSCALAR MESONS [PDF]
Photon 2001, 2002 4 pages, 1 figure (using LATEX with ws-p8-50x6-00.cls), talk presented at the International Conference on the Structure and Interactions of the Photon (PHOTON2001), Ascona, September ...
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Weak decays of $$B_c$$ Bc into two hadrons under flavor SU(3) symmetry
European Physical Journal C: Particles and Fields, 2018 A large number of $$B_c$$ Bc meson events have been recorded at the LHCb detector, especially some two-body hadronic decay modes. We analyzed the weak decays of the $$B_c$$ Bc meson into two hadron states under the flavor SU(3) symmetry.
Ruilin Zhu +3 more
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European Physical Journal C: Particles and Fields, 2020 We investigate the most interesting decay processes involving axions, photons and the lightest pseudoscalar mesons, making use of a chiral effective Lagrangian model with $$L=3$$ L=3 light quark flavors, which also includes the flavor-singlet ...
Giacomo Landini, Enrico Meggiolaro
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Meson Screening Masses in Thermal QCD
EPJ Web of Conferences, 2012 The quark-gluon plasma (QGP) excitations, corresponding to the scalar and pseudoscalar meson quantum numbers, for different temperatures are calculated.
Czerski Piotr
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B0 and Bs0 decays into J/ψ f0(980) and J/ψ f0(500) and the nature of the scalar resonances
Physics Letters B, 2014 We describe the B0 and Bs0 decays into J/ψ f0(500) and J/ψ f0(980) by taking into account the dominant process for the weak decay of B0 and Bs0 into J/ψ and a qq¯ component.
W.H. Liang, E. Oset
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Chiral Structure of Scalar and Pseudoscalar Mesons [PDF]
Advances in High Energy Physics, 2013 45 pages, 7 figures, 7 tables, to appear in Advances in High Energy ...
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European Physical Journal C: Particles and Fields, 2017 Based on the predictions of the relevant form factors from the covariant light-front quark model, we show the branching fractions for the $$D (D_s) \rightarrow (P,\,S,\,V,\,A)\,\ell \nu _\ell $$ D ( D s ) → ( P , S , V , A ) ℓ ν ℓ ( $$\ell =e$$ ℓ = e or $
Hai-Yang Cheng, Xian-Wei Kang
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Composition of the pseudoscalar η and η′ mesons [PDF]
Journal of High Energy Physics, 2007 The composition of the eta and eta' mesons has long been a source of discussion and is of current interest with new experimental results appearing. We investigate what can be learnt from a number of different processes: V to P gamma and P to V gamma (V and P are light vector and pseudoscalar mesons respectively), P to gamma gamma, J/psi,psi' to P gamma,
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