Search for the semi-leptonic decays And

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doi:10.1016/j.physletb.2023.137993
Search for the semi-leptonic decays And

M. Ablikim (Institute of High Energy Physics, Beijing, People's Republic of China) ; M.N. Achasov (G.I. Budker Institute of Nuclear Physics SB RAS (BINP), Novosibirsk, Russia) ; P. Adlarson (Uppsala University, Box 516, Uppsala, Sweden) ; R. Aliberti (Johannes Gutenberg University of Mainz, Johann-Joachim-Becher-Weg 45, Mainz, Germany) ; A. Amoroso (University of Turin, INFN, Italy; University of Turin, Turin, Italy; INFN, Turin, Italy) ; et al. - Show all 607 authors
We search for the semi-leptonic decays $Λ_{c}^{+} \to Λ π^{+} π^{-} e^{+} ν_{e}$ and $Λ_{c}^{+} \to p K_{S}^{0} π^{-} e^{+} ν_{e}$ in a sample of 4.5 ${fb}^{- 1}$ of $e^{+} e^{-}$ annihilation data collected in the center-of-mass energy region between 4.600GeV and 4.699GeV by the BESIII detector at the BEPCII. No significant signals are observed, and the upper limits on the decay branching fractions are set to be $B (Λ_{c}^{+} \to Λ π^{+} π^{-} e^{+} ν_{e}) < 3.9 \times 10^{- 4}$ and $B (Λ_{c}^{+} \to p K_{S}^{0} π^{-} e^{+} ν_{e}) < 3.3 \times 10^{- 4}$ at the 90% confidence level, respectively.
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    {
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    {
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        {
          "country": "China", 
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    {
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        {
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        {
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        {
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    {
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    {
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        {
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        {
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          "value": "Chung-Ang University, Seoul, Republic of Korea"
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        {
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    {
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        {
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          "value": "INFN Sezione di Ferrara, Ferrara, Italy"
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          "value": "Bochum Ruhr-University, Bochum, Germany"
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        {
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    {
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        {
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          "value": "Shandong University, Jinan, People's Republic of China"
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    {
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        {
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        {
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        {
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          "value": "Helmholtz Institute Mainz, Staudinger Weg 18, Mainz, Germany"
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        {
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          "value": "Bochum Ruhr-University, Bochum, Germany"
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        {
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        {
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        {
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    {
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        {
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          "value": "University of Turin, INFN, Italy"
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        {
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        {
          "country": "Italy", 
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    {
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        {
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        {
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        {
          "country": "Italy", 
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    {
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        {
          "country": "China", 
          "value": "University of Jinan, Jinan, People's Republic of China"
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        {
          "country": "China", 
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    {
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        {
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        {
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    {
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        {
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    {
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        {
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        {
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        {
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        {
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        {
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        {
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        {
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        {
          "country": "China", 
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    {
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        {
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        {
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    {
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        {
          "country": "China", 
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        {
          "country": "China", 
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        {
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        {
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        {
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    {
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        {
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          "value": "University of Turin, INFN, Italy"
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        {
          "country": "Italy", 
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        {
          "country": "Italy", 
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        {
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    {
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        {
          "country": "Italy", 
          "value": "INFN Laboratori Nazionali di Frascati, Frascati, Italy"
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    {
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        {
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          "value": "Bochum Ruhr-University, Bochum, Germany"
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    {
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        {
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          "value": "University of Muenster, Wilhelm-Klemm-Strasse 9, Muenster, Germany"
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    {
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        {
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          "value": "Institute of High Energy Physics, Beijing, People's Republic of China"
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    {
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        {
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        {
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    {
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        {
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    {
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        {
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        {
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          "value": "INFN Sezione di Ferrara, Ferrara, Italy"
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          "country": "Italy", 
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    {
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        {
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    {
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        {
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    {
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        {
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    {
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        {
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    {
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        {
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        {
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    {
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        {
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          "value": "INFN Sezione di Ferrara, Ferrara, Italy"
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        {
          "country": "Italy", 
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    {
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        {
          "country": "Italy", 
          "value": "University of Turin, INFN, Italy"
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        {
          "country": "Italy", 
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        {
          "country": "Italy", 
          "value": "INFN, Turin, Italy"
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      ], 
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        {
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        {
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    {
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        {
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    {
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        {
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    {
      "source": "Elsevier", 
      "value": "We search for the semi-leptonic decays <math><msubsup><mrow><mi>\u039b</mi></mrow><mrow><mi>c</mi></mrow><mrow><mo>+</mo></mrow></msubsup><mo>\u2192</mo><mi>\u039b</mi><msup><mrow><mi>\u03c0</mi></mrow><mrow><mo>+</mo></mrow></msup><msup><mrow><mi>\u03c0</mi></mrow><mrow><mo>\u2212</mo></mrow></msup><msup><mrow><mi>e</mi></mrow><mrow><mo>+</mo></mrow></msup><msub><mrow><mi>\u03bd</mi></mrow><mrow><mi>e</mi></mrow></msub></math> and <math><msubsup><mrow><mi>\u039b</mi></mrow><mrow><mi>c</mi></mrow><mrow><mo>+</mo></mrow></msubsup><mo>\u2192</mo><mi>p</mi><msubsup><mrow><mi>K</mi></mrow><mrow><mi>S</mi></mrow><mrow><mn>0</mn></mrow></msubsup><msup><mrow><mi>\u03c0</mi></mrow><mrow><mo>\u2212</mo></mrow></msup><msup><mrow><mi>e</mi></mrow><mrow><mo>+</mo></mrow></msup><msub><mrow><mi>\u03bd</mi></mrow><mrow><mi>e</mi></mrow></msub></math> in a sample of 4.5<math><msup><mrow><mi>fb</mi></mrow><mrow><mo>\u2212</mo><mn>1</mn></mrow></msup></math> of <math><msup><mrow><mi>e</mi></mrow><mrow><mo>+</mo></mrow></msup><msup><mrow><mi>e</mi></mrow><mrow><mo>\u2212</mo></mrow></msup></math> annihilation data collected in the center-of-mass energy region between 4.600GeV and 4.699GeV by the BESIII detector at the BEPCII. No significant signals are observed, and the upper limits on the decay branching fractions are set to be <math><mi>B</mi><mo>(</mo><msubsup><mrow><mi>\u039b</mi></mrow><mrow><mi>c</mi></mrow><mrow><mo>+</mo></mrow></msubsup><mo>\u2192</mo><mi>\u039b</mi><msup><mrow><mi>\u03c0</mi></mrow><mrow><mo>+</mo></mrow></msup><msup><mrow><mi>\u03c0</mi></mrow><mrow><mo>\u2212</mo></mrow></msup><msup><mrow><mi>e</mi></mrow><mrow><mo>+</mo></mrow></msup><msub><mrow><mi>\u03bd</mi></mrow><mrow><mi>e</mi></mrow></msub><mo>)</mo><mo>&lt;</mo><mn>3.9</mn><mo>\u00d7</mo><msup><mrow><mn>10</mn></mrow><mrow><mo>\u2212</mo><mn>4</mn></mrow></msup></math> and <math><mi>B</mi><mo>(</mo><msubsup><mrow><mi>\u039b</mi></mrow><mrow><mi>c</mi></mrow><mrow><mo>+</mo></mrow></msubsup><mo>\u2192</mo><mi>p</mi><msubsup><mrow><mi>K</mi></mrow><mrow><mi>S</mi></mrow><mrow><mn>0</mn></mrow></msubsup><msup><mrow><mi>\u03c0</mi></mrow><mrow><mo>\u2212</mo></mrow></msup><msup><mrow><mi>e</mi></mrow><mrow><mo>+</mo></mrow></msup><msub><mrow><mi>\u03bd</mi></mrow><mrow><mi>e</mi></mrow></msub><mo>)</mo><mo>&lt;</mo><mn>3.3</mn><mo>\u00d7</mo><msup><mrow><mn>10</mn></mrow><mrow><mo>\u2212</mo><mn>4</mn></mrow></msup></math> at the 90% confidence level, respectively."
    }
  ], 
  "imprints": [
    {
      "date": "2023-12-19", 
      "publisher": "Elsevier"
    }
  ]
}
Published on:: 19 December 2023
Publisher:: Elsevier
Published in:: Physics Letters B , Volume 843 C (2023)

Article ID: 137993
DOI:: https://doi.org/10.1016/j.physletb.2023.137993
Copyrights:: The Author(s)
Licence:: CC-BY-3.0
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