Repository logo
Log in(current)
Repository logoMIT Open ScholarshipDSpace@MIT
  1. Home
  2. MIT Open Access Articles
  3. MIT Open Access Articles
  4. Differential branching fraction and angular analysis of Λb0 → Λμ+μ− decays

Differential branching fraction and angular analysis of Λb0 → Λμ+μ− decays

Thumbnail Image
Download
Name

13130_2015_Article_1506.pdf

Size

800.14 KB

Format

Adobe PDF

Checksum (MD5)

fecfb9c79fd8af5541e245e05b61b735

Download all files submitted through automated deposit
art_6489779386469908183.zip (590.63 KB)
Author(s)
Aaij, R.
•
Adeva, B.
•
Adinolfi, M.
•
Affolder, A.
•
Ajaltouni, Z.
•
Akar, S.
•
Albrecht, J.
•
Alessio, F.
•
Alexander, M.
•
Ali, S.
more
Date Issued
June 2015
Journal
Journal of High Energy Physics
Publisher
Springer Berlin Heidelberg
Version
Final published version
Abstract
Abstract The differential branching fraction of the rare decay Λ b 0  → Λμ+μ− is measured as a function of q2, the square of the dimuon invariant mass. The analysis is performed using proton-proton collision data, corresponding to an integrated luminosity of 3.0 fb−1, collected by the LHCb experiment. Evidence of signal is observed in the q2 region below the square of the J/ψ mass. Integrating over 15 < q2 < 20 GeV2/c4 the differential branching fraction is measured as d ℬ Λ b 0 → Λ μ + μ − / d q 2 = 1.18 − 0.08 + 0.09 ± 0.03 ± 0.27 × 10 − 7 GeV 2 / c 4 − 1 , $$ \mathrm{d}\mathrm{\mathcal{B}}\left({\varLambda}_b^0\to \varLambda {\mu}^{+}{\mu}^{-}\right)/d{q}^2=\left({1.18}_{-0.08}^{+0.09}\pm 0.03\pm 0.27\right)\times {10}^{-7}{\left({\mathrm{GeV}}^2/{c}^4\right)}^{-1}, $$ where the uncertainties are statistical, systematic and due to the normalisation mode, Λ b 0  → J/ψΛ, respectively. In the q2 intervals where the signal is observed, angular distributions are studied and the forward-backward asymmetries in the dimuon (A FB ℓ ) and hadron (A FB h ) systems are measured for the first time. In the range 15 < q2 < 20 GeV2/c4 they are found to be A F B ℓ = − 0.05 ± 0.09 stat ± 0.03 syst and A F B h = − 0.29 ± 0.07 stat ± 0.03 syst . $$ \begin{array}{l}{A}_{\mathrm{FB}}^{\ell }=-0.05\pm 0.09\left(\mathrm{stat}\right)\pm 0.03\left(\mathrm{syst}\right)\;\mathrm{and}\hfill \\ {}{A}_{\mathrm{FB}}^h=-0.29\pm 0.07\left(\mathrm{stat}\right)\pm 0.03\left(\mathrm{syst}\right).\hfill \end{array} $$
MIT Department
Massachusetts Institute of Technology. Department of Physics
Terms of Use
Creative Commons Attribution 4.0 International license
https://creativecommons.org/licenses/by/4.0/
Persistent DSpace Link
https://hdl.handle.net/1721.1/131262
DOI of Published Version
https://doi.org/10.1007/JHEP06(2015)115
Repository logo
PrivacyPermissionsAccessibilityContact us
Repository logo
Notify us about copyright concerns.