Exotic meson

Non-quark model mesons consist of

1. Exotic mesons, which have quantum numbers not possible for mesons in the quark model
2. glueballs or gluonium, which have no valence quarks at all
3. tetraquarks, which have two valence quark-antiquark pairs,
4. and hybrid mesons, which contain a valence quark-antiquark pair and one or more gluons.

All of these can be classed as mesons, because they are hadrons and carry zero baryon number. Of these, glueballs must be flavour singlets, ie, have vanishing isospin (I=0) and strangeness. Like all particle states, they are specified by the quantum numbers which label representations of the Poincare symmetry, ie, J^PC (where J is the angular momentum, P is the intrinsic parity and C is the charge conjugation parity) and by the mass. One also specifies the isospin I of the meson.

Typically, every quark model meson comes in SU(3) flavour nonets— an octet and a flavour singlet. A glueball shows up as an extra (supernumerary) particle outside the nonet. In spite of such seemingly simple counting, the assignment of any given state as a glueball, tetraquark or hybrid remains tentative even today. Even when there is agreement that one of several states is one of these non-quark model mesons, the degree of mixing, and the precise assignment is fraught with uncertainties. There is also the considerable experimental labour of assigning quantum numbers to each state and cross checking them in other experiments. As a result, all assignments outside the quark model are tentative. The remainder of this article outlines the situation as it stood at the end of 2004.

Lattice predictions

Lattice QCD predictions for glueballs are now fairly stable, at least when virtual quarks are neglected. The two lowest states are

0^{+ +} with mass of 1611±163 MeV

2^{+ +} with mass of 2232±310 MeV

The 0^{- +} and exotic glueballs such as 0^{- -} are all expected to lie above 2 GeV. Glueballs are necessarily isoscalar, ie, have isospin I=0.

The ground state hybrid mesons — 0^{- +}, 1^{- +}, 1^{- -} and 2^{- +} all lie a little below 2 GeV. The hybrid with exotic quantum numbers 1^{- +} is at 1.9±0.2 GeV. The best lattice computations to date are made in the quenched approximation, which neglects virtual quarks loops. As a result, these computations miss mixing with meson states.

The 0^{+ +} states

The data shows five isoscalar resonances—

f₀(600), f₀(980), f₀(1370), f₀(1500) and f₀(1710)

Of these the f₀(600) is usually identified with the σ of chiral models. The decays and production of f₀(1710) give strong evidence that it is also a meson.

Glueball candidate

The f₀(1370) and f₀(1500) cannot both be a quark model meson, because one is supernumerary. The production of the higher mass state in two photon reactions such as 2γ → 2π or 2γ → 2K reactions is highly suppressed. The decays also give some evidence that one of these could be a glueball.

Tetraquark candidate

The f₀(980) has been identified by some authors as a tetraquark meson, along with the I=1 states a₀(980) and κ₀(800).Two longlived (narrow in the jargon of particle spectroscopy) states: the scalar (o⁺⁺) state <b>D_sJ(2317)^*&plmn; and the vector (1⁺) meson <b>D_sJ(2460)^*&plmn; , observed at CLEO and BaBar, have also been tentatively identified as tetraquark states. However, for these, other explanations are possible.

The 2^{+ +} states

Two isoscalar states are definitely identified— f₂(1270) and the f'₂(1525). No other states have been consistently identified by all experiments. Hence it is difficult to say more about these states.

The 1^{- +} exotics and other states

The two isovector exotics π₁(1400) and π₁(1600) seems to be well established experimentally. They are clearly not glueballs, but could be either a tetraquark or a hybrid. The evidence for such assignments is weak.

The 0^{- +} π(1800), 1^{- -} ρ(1900) and the 2^{- +} η_2<(1870) are fairly well identified states, which have been tentatively identified as hybrids by some authors. If this identification is correct, then it is a remarkable agreement with lattice computations, which place several hybrids in this range of masses.

See also

• Quark model, mesons, baryons, quarks and gluons
• Exotics and exotic baryons
• Quantum chromodynamics, flavour and the QCD vacuum

References and external links

• Particle Data Group: non quark-antiquark candidates (http://pdg.lbl.gov/2004/reviews/mxxx050.pdf) (S. Eidelman et al, Physics Letters B 592, 2004, p 1)

he:מזון אקזוטי (חלקיק)