English

X(3872) and Y(4140) using diquark-antidiquark operators with lattice QCD

High Energy Physics - Lattice 2015-11-02 v1 High Energy Physics - Phenomenology

Abstract

We discuss a recent lattice study of charmonium-like mesons with JPC=1++J^{PC}=1^{++} and three quark contents cˉcdˉu\bar cc\bar du, cˉc(uˉu+dˉd)\bar cc(\bar uu + \bar dd) and cˉcsˉs\bar cc\bar ss, where the latter two can mix with cˉc\bar cc. In this quantum channel, the long known exotic candidate, X(3872), resides. This simulation employs Nf=2N_f=2, mπ=266 m_\pi=266~MeV and a large basis of cˉc\bar cc, two-meson and diquark-antidiquark interpolating fields, with diquarks in both anti-triplet and sextet color representations. It aims at the possible signatures of four-quark exotic states. Along the way, we discuss the relations between the diquark-antidiquark operators and the two-meson operators via the Fierz transformations.

Keywords

Cite

@article{arxiv.1510.09150,
  title  = {X(3872) and Y(4140) using diquark-antidiquark operators with lattice QCD},
  author = {M. Padmanath and C. B. Lang and S. Prelovsek},
  journal= {arXiv preprint arXiv:1510.09150},
  year   = {2015}
}

Comments

7 pages, Talk given at the 33rd International Symposium on Lattice Field Theory (Lattice 2015), 14-18 July 2015, Kobe International Conference Center, Kobe, Japan