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dc.contributor.authorCooper, LJ
dc.contributor.authorDavies, CTH
dc.contributor.authorWingate, M
dc.date.accessioned2022-01-29T00:31:09Z
dc.date.available2022-01-29T00:31:09Z
dc.date.issued2022
dc.identifier.issn2470-0010
dc.identifier.urihttps://www.repository.cam.ac.uk/handle/1810/333414
dc.description.abstractWe present results of the first lattice QCD calculations of the weak matrix elements for the decays $B_c^+ \to D^0 \ell^+ \nu_{\ell}$, $B_c^+ \to D_s^+ \ell^+ \ell^-$ and $B_c^+ \to D_s^+ \nu \overline{\nu}$. Form factors across the entire physical $q^2$ range are then extracted and extrapolated to the continuum limit with physical quark masses. Results are derived from correlation functions computed on MILC Collaboration gauge configurations with three different lattice spacings and including 2+1+1 flavours of sea quarks in the Highly Improved Staggered Quark (HISQ) formalism. HISQ is also used for all of the valence quarks. The uncertainty on the decay widths from our form factors is similar in size to that from the present value for $V_{ub}$. We obtain the ratio $\Gamma (B_{c}^{+} \rightarrow D^0 \mu^{+} \nu_{\mu}) /\left|\eta_{\mathrm{EW}} V_{u b}\right|^{2}=4.43(63) \times 10^{12} \mathrm{~s}^{-1}$. Combining our form factors with those found previously by HPQCD for $B_{c}^{+} \rightarrow J / \psi \mu^{+} \nu_{\mu}$, we find $\left|V_{cb}/V_{ub} \right|^2 \Gamma( B_c^+ \to D^0 \mu^+ \nu_\mu )/\Gamma(B_{c}^{+} \rightarrow J / \psi \mu^{+} \nu_{\mu}) = 0.257(36)_{B_c \to D}(18)_{B_c \to J/\psi}$. We calculate the differential decay widths of $B_c^+ \to D_s^+ \ell^+ \ell^-$ across the full $q^2$ range, and give integrated results in $q^2$ bins that avoid possible effects from charmonium and $u \overline{u}$ resonances. For example, we find that the ratio of differential branching fractions integrated over the range $q^2 = 1 \; \mathrm{GeV}^2 - 6 \; \mathrm{GeV}^2$ for $B_c^+ \to D_s^+ \mu^+ \mu^-$ and $B_{c}^{+} \rightarrow J / \psi \mu^{+} \nu_{\mu}$ is $5.23{\tiny }(73)_{B_c \to D_s}(54)_{B_c \to J/\psi} \times 10^{-6}$. We also give results for the branching fraction of $B_c^+ \to D_s^+ \nu \overline{\nu}$. Prospects for reducing our errors in the future are discussed.
dc.publisherAmerican Physical Society (APS)
dc.rightsAttribution 4.0 International
dc.rights.urihttps://creativecommons.org/licenses/by/4.0/
dc.subjecthep-lat
dc.subjecthep-lat
dc.subjecthep-ph
dc.titleForm factors for the processes Bc+ →d0ℓ+νℓ and Bc+ → Ds+ ℓ+ℓ- (ν ν ¯) from lattice QCD FORM FACTORS for the PROCESSES Bc+ →d0ℓ+νℓ ⋯ COOPER, DAVIES, and WINGATE
dc.typeArticle
dc.publisher.departmentDepartment of Applied Mathematics And Theoretical Physics
dc.date.updated2022-01-28T16:16:33Z
prism.issueIdentifier1
prism.numberARTN 014503
prism.publicationDate2022
prism.publicationNamePhysical Review D
prism.startingPage014503
prism.volume105
dc.identifier.doi10.17863/CAM.80838
dcterms.dateAccepted2021-12-06
rioxxterms.versionofrecord10.1103/PhysRevD.105.014503
rioxxterms.versionVoR
dc.contributor.orcidWingate, Matthew [0000-0001-6568-988X]
dc.identifier.eissn2470-0029
dc.publisher.urlhttp://dx.doi.org/10.1103/PhysRevD.105.014503
rioxxterms.typeJournal Article/Review
pubs.funder-project-idScience and Technology Facilities Council (ST/P000681/1)
pubs.funder-project-idScience and Technology Facilities Council (ST/R002452/1)
pubs.funder-project-idScience and Technology Facilities Council (ST/R00689X/1)
pubs.funder-project-idScience and Technology Facilities Council (ST/M007065/1)
pubs.funder-project-idSTFC (ST/M007073/1)
pubs.funder-project-idSTFC (ST/T000694/1)
cam.issuedOnline2022-01-05
cam.depositDate2022-01-28
pubs.licence-identifierapollo-deposit-licence-2-1
pubs.licence-display-nameApollo Repository Deposit Licence Agreement


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Except where otherwise noted, this item's licence is described as Attribution 4.0 International