Cross-sections for resonance production in% MathType!MTEF!2!1!+-% feaafiart1ev1aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn% hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr% 4rNCHbGeaGak0df9q8qqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq-Jc9% vqaqpepi0xc9as0-LqLs-Jirpepeea0-as0Fb9pgea0lrP0xe9Fve9% Fve9qapdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWexLMBb50ujb% qeguuDJXwAKbacfaGaf8hCaaNbaebacqWFUbGBaaa!413C! annihilation around 2190 MeV centre-of-mass energyannihilation around 2190 MeV centre-of-mass energy
2007
Resonance production cross-sections in nonstrange annihilation channels have been studied in the c.m. energy interval from 2.13 to 2.29 GeV where the first bump in the\(\bar {\mathcal{N}} \mathcal{N}\) cross-section forI = 1 had been observed. None of the resonance intermediate states we have analysed shows a structure large enough to be mainly responsible for the enhancement.
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