2017
DOI: 10.1103/physrevd.96.075038
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Minimal flavored U(1) for B -meson anomalies

Abstract: We consider an anomaly-free U (1) model with favorable couplings to heavy flavors in the Standard Model(SM), as motivated by B-meson anomalies at LHCb. Taking the, we can explain the B-meson anomalies without invoking extra charged fermions or flavor violation beyond the SM. We show that there is a viable parameter space with a small x that is compatible with other meson decays, tau lepton and neutrino experiments as well as the LHC dimuon searches. We briefly discuss the prospects of discovering the Z gauge b… Show more

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Cited by 48 publications
(52 citation statements)
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“…For instance, we take two trajectories with p yi 1 = −p yi 2 and p zi 1,2 = 0, which contribute to the ridge (p y = 0, p z = −T z +p C ) and have δp C z 1 = δp C z 2 , yielding ∆ϕ = 0 according to Eq. (11). In this way the remarkable relation between the main lobe of the quantum interference pattern and the PMD ridge due to Coulomb focusing is confirmed.…”
Section: The Nondipole Shift Of the Main Lobesupporting
confidence: 56%
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“…For instance, we take two trajectories with p yi 1 = −p yi 2 and p zi 1,2 = 0, which contribute to the ridge (p y = 0, p z = −T z +p C ) and have δp C z 1 = δp C z 2 , yielding ∆ϕ = 0 according to Eq. (11). In this way the remarkable relation between the main lobe of the quantum interference pattern and the PMD ridge due to Coulomb focusing is confirmed.…”
Section: The Nondipole Shift Of the Main Lobesupporting
confidence: 56%
“…This follows from Eqs. (11) and (14), and the condition δp C z 1 + δp C z 2 = 0, fulfilled for these trajectories. In the case of multiple recollisions (at small values of the final |p x |), the ridge position is closer to zero: p (0) z = −T z +p C , wherep C is positive and determined by multiple recollisions, see Eq.…”
Section: The Nondipole Shift Of the Main Lobementioning
confidence: 86%
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“…In extended Higgs models, the leading contribution arises from the two-loop level Barr-Zee type diagram [180][181][182][183][184][185][186][187][188][189][190][191][192][193][194]. For supersymmetric models, a large contribution is generated from the one-loop level diagram [11,[195][196][197][198][199][200][201][202][203][204][205], together with the two-loop level diagrams [11,[206][207][208][209][210][211][212][213].…”
Section: B Chiral Perturbation Analysismentioning
confidence: 99%
“…Atoms and molecules irradiated by an intense laser pulse can produce high-order harmonic generation (HHG) [1][2][3][4][5][6][7][8][9][10][11][12][13]. Under the influence of the strong laser field, an electron can be ionized from the bound state, and accelerated in the continuum state, finally it can recombine with the ion and gives rise to the emission of extreme ultraviolet (XUV) radiation [10,14].…”
Section: Introductionmentioning
confidence: 99%