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  • Letter
  • Open Access

Measurements of Born cross sections for e+eΛc+Λ¯c(2595)+c.c. and e+eΛc+Λ¯c(2625)+c.c. at s=4918.0 and 4950.9 MeV

M. Ablikim et al. (BESIII Collaboration)
Phys. Rev. D 109, L071104 – Published 30 April 2024

Abstract

Using e+e collision data collected with the BESIII detector operating at the BEPCII collider, the Born cross sections of e+eΛc+Λ¯c(2595)+c.c. and e+eΛc+Λ¯c(2625)+c.c. are measured for the first time at center-of-mass energies of s=4918.0 and 4950.9 MeV. Nonzero cross sections are observed very close to the production threshold. The measured Born cross sections of e+eΛc+Λ¯c(2625)+c.c. are about 2–3 times greater than those of e+eΛc+Λ¯c(2595)+c.c., providing the similar behavior as semileptonic decays of Λb0, but different behavior from that in the hadronic decays of Λb0. The Born cross sections are 15.6±3.1±0.9pb and 29.4±3.7±2.7pb for e+eΛc+Λ¯c(2595)+c.c., and are 43.4±4.0±4.1pb and 76.8±6.5±4.2pb for e+eΛc+Λ¯c(2625)+c.c. at s=4918.0 and 4950.9 MeV, respectively. Based on the polar angle distributions of the Λ¯c(2625) and Λc(2625)+, the form-factor ratios |GE|2+3|GM|2/|GC| are determined for e+eΛc+Λ¯c(2625)+c.c. for the first time, which are 5.95±4.07±0.15 and 0.94±0.32±0.02 at s=4918.0 and 4950.9 MeV, respectively. All of these first uncertainties are statistical and second systematic.

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  • Received 15 December 2023
  • Accepted 2 April 2024

DOI:https://doi.org/10.1103/PhysRevD.109.L071104

Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article’s title, journal citation, and DOI. Funded by SCOAP3.

Published by the American Physical Society

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Vol. 109, Iss. 7 — 1 April 2024

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  • Figure 1
    Figure 1

    The MpKπ+ distributions of the Λc+ candidates at s= (a) 4918.0 and (b) 4950.9 MeV, where the shaded histograms is the qq¯ contribution derived from the inclusive MC samples. The region between the blue arrows is the signal region, and the regions between two neighbor green arrows are the sideband regions.

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  • Figure 2
    Figure 2

    The recoiling mass distributions MΛc+rec of the Λc+ candidates at s= (a) 4918.0 and (b) 4950.9 MeV, where the shaded histograms are the events in the MpKπ+ sideband regions in data. The blue solid lines are the total fit curves, including the signal contributions of e+eΛc+Λ¯c(2595)+c.c. and e+eΛc+Λ¯c(2625)+c.c., and the background contributions of qq¯, e+eΣcΣ¯c, and e+eΛc+Σ¯cπ+c.c. The blue dashed lines are the contributions of e+eΛc+Σ¯cπ+c.c. Other lines label individual ones.

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  • Figure 3
    Figure 3

    (a) The Born cross sections of e+eΛc+Λ¯c(2595)+c.c. and e+eΛc+Λ¯c(2625)+c.c. and the fits using Eq. (3). (b) The efficiency-corrected polar angle distributions of e+eΛc+Λ¯c(2625)+c.c. and the fits with the f(cosθ) function.

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