Search for the Rare Decays Bs0→e+e− and B0→e+e−

Aaij, R.; Abellán Beteta, C.; Ackernley, T.; Adeva, B.; Adinolfi, M.; Afsharnia, H.; Aidala, C. A.; Aiola, S.; Ajaltouni, Z.; Akar, S.; Albicocco, P.; Albrecht, J.; Alessio, F.; Alexander, M.; Alfonso Albero, A.; Alkhazov, G.; Alvarez Cartelle, P.; Alves, A. A.; Amato, S.; Amhis, Y.; An, L.; Anderlini, L.; Andreassi, G.; Andreotti, M.; Archilli, F.; Artamonov, A.; Artuso, M.; Arzymatov, K.; Aslanides, E.; Atzeni, M.; Audurier, B.; Bachmann, S.; Back, J. J.; Baker, S.; Balagura, V.; Baldini, W.; Baranov, A.; Barlow, R. J.; Barsuk, S.; Barter, W.; Bartolini, M.; Baryshnikov, F.; Basels, J. M.; Bassi, G.; Batozskaya, V.; Batsukh, B.; Battig, A.; Bay, A.; Becker, M.; Bedeschi, F.; Bediaga, I.; Beiter, A.; Belavin, V.; Belin, S.; Bellee, V.; Belous, K.; Belyaev, I.; Bencivenni, G.; Ben-Haim, E.; Benson, S.; Berezhnoy, A.; Bernet, R.; Berninghoff, D.; Bernstein, H. C.; Bertella, C.; Bertholet, E.; Bertolin, A.; Betancourt, C.; Betti, F.; Bettler, M. O.; Bezshyiko, Ia.; Bhasin, S.; Bhom, J.; 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Ramos Pernas, M.; Rangel, M. S.; Ratnikov, F.; Raven, G.; Reboud, M.; Redi, F.; Reiss, F.; Remon Alepuz, C.; Ren, Z.; Renaudin, V.; Ricciardi, S.; Richards, D. S.; Richards, S.; Rinnert, K.; Robbe, P.; Robert, A.; Rodrigues, A. B.; Rodrigues, E.; Rodriguez Lopez, J. A.; Roehrken, M.; Rollings, A.; Romanovskiy, V.; Romero Lamas, M.; Romero Vidal, A.; Roth, J. D.; Rotondo, M.; Rudolph, M. S.; Ruf, T.; Ruiz Vidal, J.; Ryzhikov, A.; Ryzka, J.; Saborido Silva, J. J.; Sagidova, N.; Sahoo, N.; Saitta, B.; Sanchez Gras, C.; Sanchez Mayordomo, C.; Santacesaria, R.; Santamarina Rios, C.; Santimaria, M.; Santovetti, E.; Sarpis, G.; Sarpis, M.; Sarti, A.; Satriano, C.; Satta, A.; Saur, M.; Savrina, D.; Scantlebury Smead, L. G.; Schael, S.; Schellenberg, M.; Schiller, M.; Schindler, H.; Schmelling, M.; Schmelzer, T.; Schmidt, B.; Schneider, O.; Schopper, A.; Schreiner, H. F.; Schubiger, M.; Schulte, S.; Schune, M. H.; Schwemmer, R.; Sciascia, B.; Sciubba, A.; Sellam, S.; Semennikov, A.; Sergi, A.; 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doi:10.1103/PhysRevLett.124.211802
Search for the Rare Decays $B_{s}^{0} \to e^{+} e^{-}$ and $B^{0} \to e^{+} e^{-}$

R. Aaij (Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands) ; C. Abellán Beteta (Physik-Institut, Universität Zürich, Zürich, Switzerland) ; T. Ackernley (Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom) ; B. Adeva (Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain) ; M. Adinolfi (H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom) ; et al. - Show all 908 authors
A search for the decays $B_{s}^{0} \to e^{+} e^{-}$ and $B^{0} \to e^{+} e^{-}$ is performed using data collected with the LHCb experiment in proton-proton collisions at center-of-mass energies of 7, 8, and 13 TeV, corresponding to integrated luminosities of 1, 2, and $2 {fb}^{- 1}$ , respectively. No signal is observed. Assuming no contribution from $B^{0} \to e^{+} e^{-}$ decays, an upper limit on the branching fraction $B (B_{s}^{0} \to e^{+} e^{-}) < 9.4 (11.2) \times 10^{- 9}$ is obtained at 90(95)% confidence level. If no $B_{s}^{0} \to e^{+} e^{-}$ contribution is assumed, a limit of $B (B^{0} \to e^{+} e^{-}) < 2.5 (3.0) \times 10^{- 9}$ is determined at 90(95)% confidence level. These upper limits are more than one order of magnitude lower than the previous values.
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      "source": "APS", 
      "title": "Search for the Rare Decays <math><mrow><msubsup><mrow><mi>B</mi></mrow><mrow><mi>s</mi></mrow><mrow><mn>0</mn></mrow></msubsup><mo>\u2192</mo><msup><mrow><mi>e</mi></mrow><mrow><mo>+</mo></mrow></msup><msup><mrow><mi>e</mi></mrow><mrow><mo>\u2212</mo></mrow></msup></mrow></math> and <math><mrow><msup><mrow><mi>B</mi></mrow><mrow><mn>0</mn></mrow></msup><mo>\u2192</mo><msup><mrow><mi>e</mi></mrow><mrow><mo>+</mo></mrow></msup><msup><mrow><mi>e</mi></mrow><mrow><mo>\u2212</mo></mrow></msup></mrow></math>"
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      "license": "CC-BY-4.0"
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    {
      "holder": "CERN", 
      "statement": "\u00a9 2020 CERN, for the LHCb Collaboration", 
      "year": "2020"
    }
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  "control_number": "54974", 
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      "source": "APS", 
      "value": "A search for the decays <math><mrow><msubsup><mrow><mi>B</mi></mrow><mrow><mi>s</mi></mrow><mrow><mn>0</mn></mrow></msubsup><mo>\u2192</mo><msup><mrow><mi>e</mi></mrow><mrow><mo>+</mo></mrow></msup><msup><mrow><mi>e</mi></mrow><mrow><mo>\u2212</mo></mrow></msup></mrow></math> and <math><mrow><msup><mrow><mi>B</mi></mrow><mrow><mn>0</mn></mrow></msup><mo>\u2192</mo><msup><mrow><mi>e</mi></mrow><mrow><mo>+</mo></mrow></msup><msup><mrow><mi>e</mi></mrow><mrow><mo>\u2212</mo></mrow></msup></mrow></math> is performed using data collected with the LHCb experiment in proton-proton collisions at center-of-mass energies of 7, 8, and 13 TeV, corresponding to integrated luminosities of 1, 2, and <math><mrow><mn>2</mn><mtext> </mtext><mtext> </mtext><msup><mrow><mi>fb</mi></mrow><mrow><mo>\u2212</mo><mn>1</mn></mrow></msup></mrow></math>, respectively. No signal is observed. Assuming no contribution from <math><mrow><msup><mrow><mi>B</mi></mrow><mrow><mn>0</mn></mrow></msup><mo>\u2192</mo><msup><mrow><mi>e</mi></mrow><mrow><mo>+</mo></mrow></msup><msup><mrow><mi>e</mi></mrow><mrow><mo>\u2212</mo></mrow></msup></mrow></math> decays, an upper limit on the branching fraction <math><mrow><mi>B</mi><mo>(</mo><msubsup><mrow><mi>B</mi></mrow><mrow><mi>s</mi></mrow><mrow><mn>0</mn></mrow></msubsup><mo>\u2192</mo><msup><mrow><mi>e</mi></mrow><mrow><mo>+</mo></mrow></msup><msup><mrow><mi>e</mi></mrow><mrow><mo>\u2212</mo></mrow></msup><mo>)</mo><mo>&lt;</mo><mn>9.4</mn><mo>(</mo><mn>11.2</mn><mo>)</mo><mo>\u00d7</mo><msup><mrow><mn>10</mn></mrow><mrow><mo>\u2212</mo><mn>9</mn></mrow></msup></mrow></math> is obtained at 90(95)% confidence level. If no <math><msubsup><mi>B</mi><mi>s</mi><mn>0</mn></msubsup><mo>\u2192</mo><msup><mi>e</mi><mo>+</mo></msup><msup><mi>e</mi><mo>\u2212</mo></msup></math> contribution is assumed, a limit of <math><mrow><mi>B</mi><mo>(</mo><msup><mrow><mi>B</mi></mrow><mrow><mn>0</mn></mrow></msup><mo>\u2192</mo><msup><mrow><mi>e</mi></mrow><mrow><mo>+</mo></mrow></msup><msup><mrow><mi>e</mi></mrow><mrow><mo>\u2212</mo></mrow></msup><mo>)</mo><mo>&lt;</mo><mn>2.5</mn><mo>(</mo><mn>3.0</mn><mo>)</mo><mo>\u00d7</mo><msup><mrow><mn>10</mn></mrow><mrow><mo>\u2212</mo><mn>9</mn></mrow></msup></mrow></math> is determined at 90(95)% confidence level. These upper limits are more than one order of magnitude lower than the previous values."
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  "imprints": [
    {
      "date": "2020-05-27", 
      "publisher": "APS"
    }
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}
Published on:: 27 May 2020
Publisher:: APS
Published in:: Physical Review Letters , Volume 124 (2020)
Issue 21
DOI:: https://doi.org/10.1103/PhysRevLett.124.211802
arXiv:: 2003.03999
Licence:: CC-BY-4.0
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