English

Radial Regge trajectories for higher $\psi(nS)$ and $\psi(nD)$ states

High Energy Physics - Phenomenology 2011-09-20 v2 High Energy Physics - Experiment

Abstract

The masses of ψ((n+1)3S1)\psi((n+1) {}^3S_1) and ψ(n3D1)\psi(n {}^3D_1) are calculated using the relativistic string Hamiltonian with "linear+gluon-exchange" potential. They occur in the range 4.5-5.8 GeV, in particular, M(3D)=4.54M(3D)=4.54 GeV, M(5S)=4.79M(5S)=4.79 GeV, M(4D)=4.85M(4D)=4.85 GeV are calculated with accuracy 50\sim 50 MeV. Linear Regge trajectories: M2(nS)=M2(ψ(4.42))+2.91M^2(nS)=M^2(\psi(4.42))+ 2.91 GeV2(n4)^2 (n-4) (n4)(n\geq 4) and M2(nD)=(4.542+2.88(n3))M^2(nD)=(4.54^2+ 2.88 (n-3)) GeV2^2 (n3n\geq 3) are obtained only for higher charmonium excitations. They have slopes two times larger than those of light mesons and give good description of calculated masses. These masses are compared with enhancements in some recent e+ee^+e^- experiments.

Keywords

Cite

@article{arxiv.1011.5580,
  title  = {Radial Regge trajectories for higher $\psi(nS)$ and $\psi(nD)$ states},
  author = {A. M. Badalian},
  journal= {arXiv preprint arXiv:1011.5580},
  year   = {2011}
}

Comments

LaTeX, 15 pages.References and short comments added. Invited paper to the special issue of Yadernaya Fizika, dedicated to the centennial anniversary of the birthday of A.B.Migdal