Abstract

Open charm hadrons with strange and non-strange mesons have been discovered in recent years. We study the spectra of several newly observed resonances by different collaborations like BaBar (del Amo Sanchez et al., Phys Rev D 82:111101, 2010) and LHCb (Aaij et al. [LHCb Collaboration], J High Energy Phys 1309:145, 2013) etc. Using an effective Lagrangian approach based on heavy quark symmetry and chiral dynamics, we explore the strong decay widths and branching ratios of various resonances and suggest their $$J^{p}$$ values. We try to fit the experimental data to find the coupling constants involved in the strong decays through pseudo-scalar mesons. The present work also discusses the possible spin–parity assignments of recently observed states by the LHCb Collaboration. The tentative assignment of the newly discovered state $$D_{J}^{*}(3000)$$ can be by natural parity states $$(0^{+},1^{-},2^{+},3^{-},\ldots )$$ , while $$D_{J}(3000)$$ can be identified with unnatural parity states like $$(0^{-},1^{+},2^{-},3^{+},\ldots )$$ . Therefore, the missing doublets 2S, 2D, 1F, 2P, and 3S can be thought of as filled up with these states. We study the two-body strong decay widths and branching ratios of missing doublets and plot the branching ratios vs. the mass of the decaying particle. These plots are used to thoroughly analyze all assignments to $$D_{J}(3000)$$ and various possibilities for the $$J^{P}$$ values.

Highlights

  • IntroductionQCD using heavy quark effective theory [3]. Collaboration [2] observed some new resonances in addition t3toheGtsheeeVeoxininsetaiasnbsotohvceeia,Dtii.o+en.πDw−iJitn(h3v0aDr02i∗0a(n)2+t4,m600aa)sn0sdsapnDedc∗Jt(Dr3u∗J0m(02.07T)60h0ea)rs0otauatnnedds iDn∗Jt(h3e00D00)π++, D2∗(2460)+, and D∗J (2760)+ were observed spectrum whereas the states measured in the

  • The hadrons containing a single heavy quark can be analyzed in a framework which is formulated for N f heavy quarks with mass m QQCD using heavy quark effective theory [3].[4]

  • We study the heavy meson decay width in the framework of heavy quark effective theory, which represents heavy quark and chiral symmetry at the chiral symmetry breaking scale χ 1 GeV [7]

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Summary

Introduction

QCD using heavy quark effective theory [3]. Collaboration [2] observed some new resonances in addition t3toheGtsheeeVeoxininsetaiasnbsotohvceeia,Dtii.o+en.πDw−iJitn(h3v0aDr02i∗0a(n)2+t4,m600aa)sn0sdsapnDedc∗Jt(Dr3u∗J0m(02.07T)60h0ea)rs0otauatnnedds iDn∗Jt(h3e00D00)π++, D2∗(2460)+, and D∗J (2760)+ were observed spectrum whereas the states measured in the. We have a heavy hadronic system containing a heavy quark with spin quantum number SQ and light degrees of freedom sl that includes light quark and gluons interacting through quark–antiquark pairs. We identify the recently observed charmed meson states D DJ (3000), and JD(2∗J5(5300)0,0D) ∗Jb(y26th0e0i)r, DJ JP (2740), D∗J (2760), assignment. These states were observed by the LHCb Collaboration and one predicted their decay widths and masses. We study the strong decays of these charmed mesons to the ground states of the heavy mesons along with the emission of pseudo-scalar pions in heavy quark effective theory in the leading order approximations.

The Lagrangian for strong decays to heavy mesons
Strong decay width formula and coupling constants
Spin-parity analysis for non-strange charm meson states
Conclusion
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