Abstract

Radiative E1 decay widths of X(3872)\rm X(3872) are calculated through the relativistic Salpeter method, with the assumption that X(3872)\rm X(3872) is the χc1χ_{c1}(2P) state, which is the radial excited state of χc1χ_{c1}(1P). We firstly calculated the E1 decay width of χc1χ_{c1}(1P), the result is in agreement with experimental data excellently, then we calculated the case of X(3872)\rm X(3872) with the assignment that it is χc1χ_{c1}(2P). Results are: $Γ({\rm X(3872)}\rightarrow γ\sl J/ψ)=33.0$ keV, Γ(X(3872)→γψ(2S))=146Γ({\rm X(3872)}\rightarrow γψ(2S))=146 keV and Γ(X(3872)→γψ(3770))=7.09Γ({\rm X(3872)}\rightarrow γψ(3770))=7.09 keV. The ratio ${{\rm Br(X(3872)}\rightarrowγψ(2{\rm S}))}/{{\rm Br(X(3872)}\rightarrow γ{\sl J}/ψ)}=4.4$ agrees with experimental data by BaBar, but larger than the new up-bound reported by Belle recently. With the same method, we also predict the decay widths: Γ(χb1(1P))→γΥ(1S))=30.0Γ(χ_{b1}(1\rm P))\rightarrow γΥ(1\rm S))=30.0 keV, Γ(χb1(2P))→γΥ(1S))=5.65Γ(χ_{b1}(2\rm P))\rightarrow γΥ(1\rm S))=5.65 keV and Γ(χb1(2P))→γΥ(2S))=15.8Γ(χ_{b1}(2\rm P))\rightarrow γΥ(2S))=15.8 keV, and the full widths: Γ(χb1(1P))∼85.7Γ(χ_{b1}(1\rm P))\sim 85.7 keV, Γ(χb1(2P))∼66.5Γ(χ_{b1}(2\rm P))\sim 66.5 keV.

Explore this paper’s authors, topics and related work.

Building this map preview

BZPEER is loading the nearby papers, people, topics and institutions for this page.

Reviews 0

Write a reviewWrite

No reviews yet.

Discussion 0

Add a commentWrite

No comments yet.