Physics – Nuclear Physics – Nuclear Theory
Scientific paper
2004-07-29
Phys.Rev. C72 (2005) 067001
Physics
Nuclear Physics
Nuclear Theory
As published in PRC 12/2005
Scientific paper
10.1103/PhysRevC.72.067001
It is argued that in the antiproton-proton annihilation into two mesons $\bar pp\longrightarrow m_1 m_2$, the origin of different restrictive angular momentum selection rules commonly obtained for planar annihilation diagrams $A2$ and for non-planar rearrangement diagrams $R2$ lies in the omission of momentum transfer between an annihilated antiquark-quark pair and a remaining quark or antiquark. If it is included, there is no reason for dismissing one type of diagram in favor of another one. Some considerations in the large $N_c$ limit of QCD equally shed light on the planar and non-planar contributions to the total $\bar NN\to m_1 m_2$ annihilation amplitude.
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