Abstract

A study of hadron production at the nucleon-antinucleon threshold has been performed with the CMD-3 detector at the VEPP-2000 e+e− collider. The very fast rise with about 1 MeV width has been observed in the e+e−→pp¯ cross section. A sharp drop in the e+e−→3(π+π−) cross section has been confirmed and found to have a less than 2 MeV width, in agreement with the observed fast rise of the e+e−→pp¯ cross section. For the first time a similar sharp drop is demonstrated in the e+e−→K+K−π+π− cross section. The behavior of the e+e−→3(π+π−),K+K−π+π− cross sections cannot be explained by an interference of any resonance amplitude with continuum, therefore this phenomenon cannot be due to a narrow near-threshold resonance. No such structure has been observed in the e+e−→2(π+π−) cross section.

Highlights

  • Production of six pions in e+e− annihilation, studied at DM2 [1,2,3], showed a “dip” in the cross section at about 1.9 GeV, confirmed later by the Fermilab E687 experiment in photoproduction [4,5], and with a much larger effective integrated luminosity at BaBar [6] using initial-state radiation (ISR)

  • In this paper we present the analysis of 50 pb−1 of integrated luminosity collected with the CMD-3 detector [18] at 29 c.m. energy points at the VEPP-2000 collider with the upgraded injection complex [19,20,21,22]

  • The energy position of the “dip” in the e+e− → K + K −π +π − cross sections, observed for the first time, is consistent with the nnproduction threshold, while that for the e+e− → 3(π +π −) reaction is close to the p pthreshold

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Summary

Introduction

Production of six pions in e+e− annihilation, studied at DM2 [1,2,3], showed a “dip” in the cross section at about 1.9 GeV, confirmed later by the Fermilab E687 experiment in photoproduction [4,5], and with a much larger effective integrated luminosity. A measurement of the CMD-3 Collaboration [8] confirmed these observations and demonstrated that the drop in the e+e− → 3(π +π −) cross section occurred in the narrow energy range of less than 10 MeV width. For the new data we have reproduced all steps for selection of four charged tracks, pion-kaon separation procedure, and the calculation of the efficiency and radiative corrections. The same overall statistical accuracy is achieved since the scan around the N Nthreshold is performed with large integrated luminosity that allows us to select about 1500 signal events per energy point. At each energy a visible cross section is calculated as the number of selected events divided by the detection efficiency and integrated luminosity. We estimate the systematic uncertainty as about 10%, dominated by the uncertainty in the efficiency calculation: a special study was performed to estimate data-MC difference in the reconstruction efficiency

The N Nthreshold region
Conclusion
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