2015
DOI: 10.1140/epjc/s10052-015-3801-2
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Prospects of discovering new physics in rare charm decays

Abstract: The LHCb bounds on the branching ratio of the rare decay D 0 → μ + μ − and the constraints on the branching ratio of D + → π + μ + μ − in the nonresonant regions enable us to improve constraints on new physics contributions. Using the effective Lagrangian approach we determine the sizes of the Wilson coefficients allowed by the existing LHCb bounds on rare charm decays. Then we discuss contributions to rare charm meson decay observables in several models of new physics: a model with an additional spin-1 weak t… Show more

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Cited by 78 publications
(155 citation statements)
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“…[80]. We learn that the ensuing bound y sµ 0.5(m S 3 /TeV) from rare decays is weaker than the abovementioned bound from semileptonic decays.…”
Section: Decaysmentioning
confidence: 90%
“…[80]. We learn that the ensuing bound y sµ 0.5(m S 3 /TeV) from rare decays is weaker than the abovementioned bound from semileptonic decays.…”
Section: Decaysmentioning
confidence: 90%
“…Nevertheless, there have been a number of phenomenological studies on the new-physics (NP) sensitivities of rare charm decays, including radiative and rare semileptonic D-meson decays induced by c → uγ and c → u + − transitions, see e.g. [4][5][6][7][8][9][10][11][12][13][14][15][16].…”
Section: Jhep08(2017)105mentioning
confidence: 99%
“…A straightforward approach, which has already been extensively used in the past [7,9,12,13,15], assumes that the long-distance hadronic effects are completely dominated by the lowest-lying narrow vector states (ρ, ω, φ etc.) which are then modelled by Breit-Wigner resonances.…”
Section: Jhep08(2017)105mentioning
confidence: 99%
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“…weaken these constraints, and following [37], we find these constraints are subdominant to those derived from mixing. We briefly note the potential importance of a dimension 6 operator beyond those considered in eq.…”
Section: Jhep01(2017)054mentioning
confidence: 51%