N. N. Achasov, E. V. Rogozina
Published 2015-01-15Version 1
Reasons are given that X(3872), I^G(J^{PC})=0^+(1^{++}), is the \chi_{1c}(2P) charmonium. Possibility of verification of this assumption is discussed.
Comments: 6 pages, 3 figures
Relations for two body B Decays to Charmonium and tests for $η-η^{\prime}$ mixing
Production of charmonium $χ_{cJ}(2P)$ plus one $ω$ meson by $e^+e^-$ annihilation
Understanding the $0^{++}$ and $2^{++}$ charmonium(-like) states near 3.9 GeV
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