Abstract:Recent high precision determinations of Vus and Vud indicate towards anomalies in the first row of the CKM matrix. Namely, determination of Vud from beta decays and of Vus from kaon decays imply a violation of first row unitarity at about 3σ level. Moreover, there is tension between determinations of Vus obtained from leptonic Kμ2 and semileptonic Kℓ3 kaon decays. These discrepancies can be explained if there exist extra vector-like quarks at the TeV scale, which have large enough mixings with the lighter quar… Show more
“…We first note that only the three representations U , D, or Q 1 (with couplings to both up and down quarks) can explain the CAA [1,[63][64][65] due to their mixing with the SM quarks, while, on the other hand, T 1 or T 2 worsen the CAA. EWPO places multi-TeV mass limits on the VLQs U , D, and Q 1 (for couplings fixed to unity), which come close to ruling out the best-fit regions from the CAA for U and D, while there is actually a small (1σ) preference for the other representations (Q 5,7 and T 1,2 ) driven by R 0 e and R 0 µ .…”
Section: Vector-like Quarksmentioning
confidence: 95%
“…While the anomalies in semi-leptonic B decays and the anomalous magnetic moment of the muon point towards NP related to second-and third-generation fermions, the CAA and the CMS di-lepton excess can be related to first-generation quarks and leptons, with simultaneous explanations possible in terms of the effective dimension-6 operator Q (3) q [62]. Similarly, explanations of the CAA via modified W -u-d couplings also require NP related to first generation-quarks [1,[63][64][65]. In this paper, we take the large array of complementary measurements sensitive to first-generation NP, together with hints for potential NP effects, as motivation to perform a combined analysis, concentrating on possible correlations among the processes listed above.…”
New-physics (NP) constraints on first-generation quark-lepton interactions are particularly interesting given the large number of complementary processes and observables that have been measured. Recently, first hints for such NP effects have been observed as an apparent deficit in first-row CKM unitarity, known as the Cabibbo angle anomaly, and the CMS excess in $$ q\overline{q} $$
q
q
¯
→ e+e−. Since the same NP would inevitably enter in searches for low-energy parity violation, such as atomic parity violation, parity-violating electron scattering, and coherent neutrino-nucleus scattering, as well as electroweak precision observables, a combined analysis is required to assess the viability of potential NP interpretations. In this article we investigate the interplay between LHC searches, the Cabibbo angle anomaly, electroweak precision observables, and low-energy parity violation by studying all simplified models that give rise to tree-level effects related to interactions between first-generation quarks and leptons. Matching these models onto Standard Model effective field theory, we derive master formulae in terms of the respective Wilson coefficients, perform a complete phenomenological analysis of all available constraints, point out how parity violation can in the future be used to disentangle different NP scenarios, and project the constraints achievable with forthcoming experiments.
“…We first note that only the three representations U , D, or Q 1 (with couplings to both up and down quarks) can explain the CAA [1,[63][64][65] due to their mixing with the SM quarks, while, on the other hand, T 1 or T 2 worsen the CAA. EWPO places multi-TeV mass limits on the VLQs U , D, and Q 1 (for couplings fixed to unity), which come close to ruling out the best-fit regions from the CAA for U and D, while there is actually a small (1σ) preference for the other representations (Q 5,7 and T 1,2 ) driven by R 0 e and R 0 µ .…”
Section: Vector-like Quarksmentioning
confidence: 95%
“…While the anomalies in semi-leptonic B decays and the anomalous magnetic moment of the muon point towards NP related to second-and third-generation fermions, the CAA and the CMS di-lepton excess can be related to first-generation quarks and leptons, with simultaneous explanations possible in terms of the effective dimension-6 operator Q (3) q [62]. Similarly, explanations of the CAA via modified W -u-d couplings also require NP related to first generation-quarks [1,[63][64][65]. In this paper, we take the large array of complementary measurements sensitive to first-generation NP, together with hints for potential NP effects, as motivation to perform a combined analysis, concentrating on possible correlations among the processes listed above.…”
New-physics (NP) constraints on first-generation quark-lepton interactions are particularly interesting given the large number of complementary processes and observables that have been measured. Recently, first hints for such NP effects have been observed as an apparent deficit in first-row CKM unitarity, known as the Cabibbo angle anomaly, and the CMS excess in $$ q\overline{q} $$
q
q
¯
→ e+e−. Since the same NP would inevitably enter in searches for low-energy parity violation, such as atomic parity violation, parity-violating electron scattering, and coherent neutrino-nucleus scattering, as well as electroweak precision observables, a combined analysis is required to assess the viability of potential NP interpretations. In this article we investigate the interplay between LHC searches, the Cabibbo angle anomaly, electroweak precision observables, and low-energy parity violation by studying all simplified models that give rise to tree-level effects related to interactions between first-generation quarks and leptons. Matching these models onto Standard Model effective field theory, we derive master formulae in terms of the respective Wilson coefficients, perform a complete phenomenological analysis of all available constraints, point out how parity violation can in the future be used to disentangle different NP scenarios, and project the constraints achievable with forthcoming experiments.
“…There are several possibilities to account for the CAA [52]. For instance, via modified W -quark couplings [34,53], a modified W − µν µ coupling [37,38,[54][55][56][57][58][59], a tree-level contribution to the muon decay [34,60,61] or by a tree-level effect in beta decays [62]. Since we aim at connecting the CAA to the CMS measurement we will focus on the latter possibility in which case only one operator, in the basis of Ref.…”
In addition to the existing strong indications for lepton flavour university violation (LFUV) in low energy precision experiments, CMS recently released an analysis of non-resonant di-lepton pairs which could constitute the first sign of LFUV in high-energy LHC searches. In this article we show that the Cabibbo angle anomaly, an (apparent) violation of first row and column CKM unitarity with ≈ 3 σ significance, and the CMS result can be correlated and commonly explained in a model independent way by the operator [Q). This is possible without violating the bounds from the non-resonant di-lepton search of ATLAS (which interestingly also observed slightly more events than expected in the electron channel) nor from R(π) = π → µν/π → eν. We find a combined preference for the new physics hypothesis of 4.5 σ and predict 1.0004 < R(π) < 1.0009 (95% CL) which can be tested in the near future with the forthcoming results of the PEN experiment.
“…Solutions to the anomaly with vector-like quarks (VLQ) and vector-like leptons (VLL) are discussed in Ref. [1,2,31,[34][35][36]. They proceed via a modification of the gauge boson couplings with quarks and leptons respectively, therefore a global fit to a large set of observables has to be performed.…”
The Cabibbo-Kobayashi-Maskawa (CKM) matrix parametrizes the misalignement between the up-and down-quark mass basis in the Standard Model (SM). The observation of first row CKM unitarity violation has recently emerged as a new anomaly of the SM, known as the "Cabibbo Angle Anomaly" (CAA). With current measurements, comparing the elements V ud and V us extracted from beta and kaon decays respectively, the tension with the SM prediction amounts to ∼3 σ. Recently, it has been pointed out that this anomaly can also be seen as a discrepancy in the determination of the Fermi constant from muon decay vs β and K decays, once CKM unitarity is assumed. In fact, possible explanations in terms on New Physics fall under two broad classes: contributions to β decay and/or to µ decay. In this proceedings, we discuss these solutions in terms of gauge invariant dimension 6 operators in SMEFT and simplified extensions of the Standard Model. The latter could introduce correlations with other anomalies in the SM, pointing to new and interesting directions for model building.
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