Partial widths of the γγ decay of the tensor q\documentclass[12pt]{minimal}
\usepackage{amsmath}
\usepackage{wasysym}
\usepackage{amsfonts}
\usepackage{amssymb}
\usepackage{amsbsy}
\usepackage{mathrsfs}
\usepackage{upgreek}
\setlength{\oddsidemargin}{-69pt}
\begin{document}
$$\bar q$$
\end{document} states a2(1320), f2(1270), and f2(1525) and their radial excitations a2(1660), f2(1640), and f2(1800), as well as 3F2q\documentclass[12pt]{minimal}
\usepackage{amsmath}
\usepackage{wasysym}
\usepackage{amsfonts}
\usepackage{amssymb}
\usepackage{amsbsy}
\usepackage{mathrsfs}
\usepackage{upgreek}
\setlength{\oddsidemargin}{-69pt}
\begin{document}
$$\bar q$$
\end{document} states, are calculated. Calculations are performed in the framework of the same approach that was used before for the study of radiative decays f0(980) → γγ, a0(980) → γγ, and φ(1020) → γf0(980): the assumption made is that of q\documentclass[12pt]{minimal}
\usepackage{amsmath}
\usepackage{wasysym}
\usepackage{amsfonts}
\usepackage{amssymb}
\usepackage{amsbsy}
\usepackage{mathrsfs}
\usepackage{upgreek}
\setlength{\oddsidemargin}{-69pt}
\begin{document}
$$\bar q$$
\end{document} structure of f0(980) and a0(980) [A.V. Anisovich et al., Phys.Lett. B 456, 80 (1999); Yad. Fiz. 65, 523 (2002)].The description of the decay partial widths for a2(1320), f2(1270), f2(1525) and f0(980), a0(980) is reached with the approximately equal radial wave functions, thus giving a strong argument in favor of the fact that these scalar and tensor mesons are to be classified as members of the same P-wave q\documentclass[12pt]{minimal}
\usepackage{amsmath}
\usepackage{wasysym}
\usepackage{amsfonts}
\usepackage{amssymb}
\usepackage{amsbsy}
\usepackage{mathrsfs}
\usepackage{upgreek}
\setlength{\oddsidemargin}{-69pt}
\begin{document}
$$\bar q$$
\end{document} multiplet.