The paper examines the radiative decay of one charged lepton into another, both with an emitted photon and through a three-lepton final state. Such processes are forbidden in the Standard Model, where lepton-flavor number is conserved, so their experimental detection would provide evidence of physics beyond the Standard Model. The authors also study the muon anomalous magnetic dipole moment, a precisely measured quantity that constrains possible contributions from new interactions.

The FDM extends the Standard Model gauge group with a local U(1) symmetry whose charges are associated with fermion flavor. It also introduces two additional scalar doublets and one scalar singlet. The third generation of fermions obtains mass through tree-level couplings to the Standard Model Higgs doublet, while the first two generations are linked to the third through tree-level mixings. A Type-I seesaw mechanism generates small Majorana neutrino masses and neutrino flavor mixings. The source describes the framework as addressing fermion flavor mixing, the fermion mass hierarchy and neutrino-mass generation within a single model.

Because the additional U(1) charges depend on flavor, the model’s new gauge interactions and Yukawa couplings can produce charged-lepton flavor violation. The particle content includes only two right-handed neutrinos with nonzero U(1) charge, leaving one active neutrino massless at tree level as a characteristic feature of the framework. The scalar sector contains two neutral Goldstone modes and one singly charged Goldstone mode, while the fermion mass matrices are constructed so that the measured quark and charged-lepton masses can be reproduced within the approximation used by the authors.

For the muon anomalous magnetic moment, the study calculates one-loop contributions from two dominant types of diagrams: loops containing neutrinos and charged Higgs bosons, and loops containing charged leptons with neutral scalar or pseudoscalar particles. The numerical analysis uses the reported experimental difference between the measured muon magnetic moment and the Standard Model prediction of 26(66) × 10^−11, corresponding to a 0.5-standard-deviation difference. This is substantially below the five-standard-deviation discovery threshold and therefore places strict limits on new-physics contributions.

The authors scan a parameter space subject to constraints on vacuum stability, perturbativity, Higgs signal strengths at the two-standard-deviation level and direct searches for additional scalars. The scan also imposes a lower limit of 4.05 TeV on the mass of the additional Z′ boson at 95% confidence level and requires M_Z′/g_F to exceed 6 TeV at 99% confidence level. The analysis finds that the predicted muon correction generally decreases as the charged Higgs mass increases, with a wider spread of values for charged Higgs masses below 100 GeV. The charged-Higgs-mediated loop gives the strongest effect among the contributions examined.

For charged-lepton flavor violation, the authors compute branching ratios for the radiative modes l_j^− → l_i^−γ and the three-lepton modes l_j^− → l_i^−l_i^−l_i^+. The dominant contributions to the latter include photon-, Z- and Z′-penguin diagrams, together with box diagrams containing fermions and scalar particles. The numerical calculation fixes several scalar, gauge and neutrino-sector parameters at values compatible with the measured Higgs mass and the latest muon g−2 result, then varies the first scalar doublet’s vacuum expectation value v_1, an electron-mass-matrix element m_e,13 and flavor-mixing phases.

The predicted branching ratios decrease as v_1 increases, showing that a larger vacuum expectation value suppresses lepton-flavor violation in the analyzed setup. At small v_1, the predictions for μ → eγ and μ → 3e exceed the corresponding present experimental upper bounds, while remaining potentially accessible to future experiments. Increasing m_e,13 strongly reduces the two muon-to-electron channels; it causes slower decreases for τ → eγ and τ → 3e, while the τ → μγ and τ → 3μ rates depend only weakly on that element. The flavor-mixing phases affect the muon-to-electron and tau-to-electron rates through their influence on mixing strength, but have a negligible effect on the two tau-to-muon channels in the reported scans.

The study’s conclusions are conditional on the model, its parameter choices and the one-loop treatment of the relevant observables. Its numerical results indicate that the FDM can reproduce current muon g−2 data over much of the scanned viable parameter space and can generate rare-decay rates within the reach of next-generation experiments. The authors did not calculate coherent μ → e conversion rates in nuclei, although they note that the model’s dipole, photon-penguin and Z/Z′-penguin contributions could also contribute to that complementary observable.

Subject of Research: Theoretical predictions for muon g−2 and charged-lepton flavor-violating decays in a flavor-dependent U(1) gauge model

Article Title: Lepton-flavor violation and muon \((g-2)\) in the flavor-dependent \(U(1)_F\) model

Article References: Peng, Y.-J., Niu, F.-Y., Qin, Q.-Z., Cao, Z., & Yang, J.-L. (2026). Lepton-flavor violation and muon $$(g-2)$$ in the flavor-dependent $$U(1)_F$$ model. The European Physical Journal C, 86(10), Article 1184. https://doi.org/10.1140/epjc/s10052-026-16457-7

Image Credits: AI Generated

DOI: 10.1140/epjc/s10052-026-16457-7

Keywords: lepton flavor violation, muon g−2, flavor-dependent U(1), rare lepton decays, muon-to-electron gamma, tau decays, Z′ boson, new physics, theoretical physics, Lepton-flavor, violation, muon

The NA62 collaboration recently announced a measurement of the branching ratio of the decay K+ → π+ ν ν̄, based on data collected between 2016 and 2024. The result, (9.6 +1.9/−1.8) × 10⁻¹¹, is fully consistent with the most precise Standard Model predictions, which the authors place at (8.65 ± 0.42) × 10⁻¹¹ using a strategy that determines the quark mixing parameters exclusively from meson mixing observables, thereby eliminating the dependence on the poorly known CKM parameter |V_cb|. A complementary global fit gives (8.55 ± 0.47) × 10⁻¹¹, and the agreement between the two approaches underscores how theoretically clean these decays are. NA62 will complete its full dataset in 2026, with roughly one third of the data still awaiting analysis, so a deviation from the Standard Model is not yet excluded.

The theoretically cleanest partner of this decay is the neutral mode KL → π⁰ ν ν̄, which has never been observed. The KOTO experiment at J-PARC in Japan is currently searching for it, and its latest upper bound of 2.2 × 10⁻⁹ at 90% confidence level sits roughly two orders of magnitude above the Standard Model prediction of (3.05 ± 0.17) × 10⁻¹¹. This enormous gap is precisely what excites theorists: the neutral decay is almost free of theoretical uncertainties because, unlike the charged mode, it receives no significant contribution from charm quark loops. KOTO is expected to improve its sensitivity by an order of magnitude by 2030, and the proposed KOTO II experiment aims to deliver the first discovery of this golden mode and measure its branching ratio in the late 2030s.

The heart of the new analysis is a model-independent study of how the two neutrino modes constrain each other. Both branching ratios depend on a single complex function, X_eff, whose magnitude and weak phase β_X encode any new physics contribution. The authors show that the NA62 measurement restricts the magnitude of X_eff to between 4.8 × 10⁻⁴ and 10.9 × 10⁻⁴, within about a factor of two of the Standard Model value of 5.3 × 10⁻⁴. If new particles couple only through left-handed or only through right-handed quark currents, the constraint from the CP-violating parameter ε_K forces the two branching ratios onto narrow correlated branches, limiting any enhancement of the neutral mode to at most a factor of five. But the picture changes radically when both handedness structures are present simultaneously.

With large new CP-violating phases and a small admixture of right-handed couplings, the charged decay can remain Standard Model-like while the neutral mode is boosted by a full order of magnitude, approaching the model-independent Grossman–Nir bound, which states that the neutral branching ratio cannot exceed 4.3 times the charged one in any scenario with Standard Model neutrinos. The mechanism relies on a delicate cancellation: an enhancement of one term in the charged decay amplitude can be compensated by a suppression of another, leaving the charged rate unchanged while the phase β_X grows to roughly 110 degrees, close to 90 degrees beyond the Standard Model value of about 24 degrees. In such a scenario, the neutral decay could even exceed the charged one in rate, a complete inversion of the Standard Model hierarchy in which the neutral mode is expected at about one third of the charged rate.

The analysis does not stop at the neutrino modes. The authors trace how the same new physics would ripple through a web of related observables. The decay KS → μ+μ−, currently bounded by LHCb at less than 2.1 × 10⁻¹⁰, about a factor of fifty above its Standard Model prediction of (5.2 ± 1.5) × 10⁻¹², can be enhanced by more than a factor of one hundred in the new scenario, placing it squarely within the reach of LHCb’s upcoming Run 3 and beyond. The rare semileptonic decays KL → π⁰ e+e− and KL → π⁰ μ+μ−, whose present KTeV bounds still exceed the Standard Model predictions of 3.5 × 10⁻¹¹ and 1.4 × 10⁻¹¹ by roughly an order of magnitude, can also be strongly enhanced, with KOTO II planning to measure the electron channel in a second phase of its programme.

To make these correlations concrete, the authors construct an explicit scenario involving a Z′ boson, a hypothetical heavy neutral gauge boson associated with a new U(1)′ gauge symmetry. A crucial technical insight, drawn from earlier work, is that the dangerous contribution of the Z′ to kaon mixing can be suppressed by a fine-tuned pattern of left- and right-handed couplings: the right-handed flavour-changing coupling must be roughly 240 times smaller than its left-handed counterpart. This tiny right-handed coupling plays a single, vital role, keeping the mixing observables ε_K and ΔM_K consistent with experiment, while the dominant left-handed coupling remains large enough to drive spectacular effects in the rare decays. The electroweak penguin operator Q8 then dominates the new contribution to the direct CP-violating ratio ε′/ε, which the Dual QCD approach estimates at only (5 ± 2) × 10⁻⁴ in the Standard Model, well below the experimental value of (16.6 ± 2.3) × 10⁻⁴, a discrepancy that would constitute one of the largest anomalies in flavour physics if confirmed.

The numerical analysis demonstrates that all the requirements can be satisfied simultaneously. With the Z′ mass fixed at 5 TeV and a representative left-handed lepton coupling of 0.5, the authors find parameter regions in which the charged decay ratio stays at unity, the neutral decay reaches the Grossman–Nir bound, the short-distance contribution to KL → μ+μ− respects its experimental bound, and the ratios for KS → μ+μ−, KL → π⁰ ℓ+ℓ− and ε′/ε are all significantly enhanced. The interplay between the sign of the interference between direct and mixing-induced CP violation in the semileptonic channels adds further structure: with positive interference, the electron channel can saturate its experimental limit, while negative interference keeps it below the bound yet still far above the Standard Model expectation. The authors also show how a future measurement of the neutral neutrino mode by KOTO II, combined with the NA62 result, would determine the magnitude and phase of X_eff, albeit with a residual four-fold ambiguity that other decays could help resolve.

The broader message is one of encouragement for the experimental kaon programme. The NA62 result, far from closing the door on new physics, reshapes the map of where it can still hide, pointing decisively toward scenarios that combine left- and right-handed couplings with new CP-violating phases. The coming decade promises a dense schedule of measurements: the final NA62 result, KOTO’s march toward sensitivity, KOTO II’s discovery target in the late 2030s, LHCb’s pursuit of KS → μ+μ−, and continued theoretical efforts to pin down the Standard Model value of ε′/ε. Together, these efforts will test whether the kaon system, the historic birthplace of CP violation, is about to deliver another revolution in our understanding of matter at the fundamental level.

Subject of Research: New physics prospects in rare and CP-violating kaon decays following the NA62 measurement of K+ → π+ ν ν̄

Article Title: Prospects for ({K_L \rightarrow \pi ^0\nu \bar{\nu }}), (K_S\rightarrow \mu ^+\mu ^-), (K_L\rightarrow \pi ^0 \ell ^+\ell ^-) and (\varepsilon '/\varepsilon ) after the new ({K^+ \rightarrow \pi ^+\nu \bar{\nu }}) result from NA62

Article References: Blanke, M., Buras, A. J., Lazzeroni, C., & Swallow, J. C. (2026). Prospects for $${K_L \rightarrow \pi ^0\nu \bar{\nu }}$$, $$K_S\rightarrow \mu ^+\mu ^-$$, $$K_L\rightarrow \pi ^0 \ell ^+\ell ^-$$ and $$\varepsilon '/\varepsilon $$ after the new $${K^+ \rightarrow \pi ^+\nu \bar{\nu }}$$ result from NA62. The European Physical Journal C, 86(10), Article 1166. https://doi.org/10.1140/epjc/s10052-026-16418-0

Image Credits: AI Generated

DOI: 10.1140/epjc/s10052-026-16418-0

Keywords: kaon decays, NA62, KOTO, KOTO II, LHCb, new physics, CP violation, Z prime boson, Standard Model, flavour physics, epsilon prime over epsilon, Grossman-Nir bound

The decays in question, written in shorthand as b to c anti-u q transitions, occupy a special place in flavour physics because they are unusually clean theoretically. In the framework known as QCD factorisation, the decay amplitudes can be computed perturbatively, and crucially, the final states contain no identical quark-antiquark pairs. That absence eliminates the so-called weak annihilation topologies, which are the dominant source of uncalculable infrared divergences and typically inflate the error budget of non-leptonic B decays. The residual power corrections, suppressed by powers of the QCD scale divided by the bottom quark mass, are expected to sit at the level of roughly one per cent. With experimental precisions now pushing below three per cent, these channels should be among the best-understood processes in the entire flavour sector, which makes the observed deviations all the more perplexing.

Theorists have proposed two broad families of explanations. The first is that the hadronic uncertainties have simply been underestimated, and that quantum chromodynamics, the theory of the strong force, is not as well controlled in these decays as the formalism suggests. The second is more tantalising: the deviations are indirect fingerprints of new particles that mediate the quark-level transition at tree level, modifying the decay amplitude before the Standard Model contribution even enters. Previous work had already shown that the simplest realisation of the new physics idea, an additional Higgs doublet coupling to quarks, runs into immediate trouble with LHC dijet searches, because the same mediator that shifts the B meson decay also produces spectacular resonances decaying to pairs of jets that the experiments have not observed.

The new study examines three plausible ways around that impasse. The first is that the new physics is top-philic, meaning the neutral component of the extra Higgs doublet preferentially decays to pairs of top quarks rather than light jets. Top-pair resonance searches are notoriously difficult, suffering from large QCD backgrounds and significant signal-background interference that limits their sensitivity. If the neutral scalar dumps most of its branching fraction into top quarks, one might reasonably hope that the dijet bounds would weaken dramatically, opening a viable window for the model. The authors extended the minimal coupling structure with a new coupling to right-handed up-type quarks, allowing the neutral scalar to decay to top pairs with branching ratios approaching unity, and then carefully recast the relevant ATLAS and CMS analyses.

The result defied expectations. Even with a large branching ratio to top quark pairs, the dijet constraints on the neutral component did not weaken in any systematic way, and in some regions of parameter space they actually became stronger. More importantly, the charged component of the doublet, which cannot hide in top final states, provides bounds that are roughly equally strong across most of the scanned parameter range. The authors used the full suite of modern dijet searches, including the CMS-EXO-21-010 analysis, which postdates and supersedes the constraints used in earlier studies, and found that the updated limits are even more restrictive than those previously reported. Hiding the new scalar in top quarks, in other words, does not reconcile the collider data with the flavour anomaly.

The second escape route involves questioning QCD itself. The authors asked how large the power corrections in the clean decays would need to be to explain the discrepancy without any new physics. To calibrate expectations, they turned to related B decays into pairs of light mesons, such as B to pi pi and B to K K, where non-factorisable contributions are known to be prominent and where recent data-driven analyses have bounded the power-suppressed annihilation terms at roughly twenty per cent at most. Since the clean channels studied here should be far less sensitive to such effects, power corrections anywhere near that size would already be surprising. Yet the analysis shows that a shift of around minus fifteen per cent would be needed to fully absorb the anomaly, and even a more moderate correction of minus ten per cent, which halves the required new physics coupling, still leaves the favoured parameter region in substantial tension with the dijet limits.

The third strategy is brute force: add more particles. If the model contains n copies of the additional Higgs doublet, each with identical couplings, their contributions to the low-energy decay amplitude add constructively while the collider signal for each individual resonance is diluted. The authors considered extensions with up to four additional doublets, a five-Higgs-doublet model, and found that even this extreme scenario remains excluded by current collider bounds when no power corrections are assumed. Only when all three mechanisms are combined, multiple doublets, top-philic neutral components and a ten per cent power correction, does a narrow viable window emerge, with degenerate doublets near a mass of 600 GeV. Even then, the model cannot fully reach the coupling strength maximally preferred by the non-leptonic data, and the authors note that a hypothetical fourteen-doublet model would be needed to evade the collider constraints entirely without power corrections.

The study also checked whether the surviving parameter space conflicts with other precision measurements. Extended Higgs sectors contribute to the decay of the Z boson to bottom quarks, to B meson mixing, to rare radiative decays, and to the lifetime ratio of charged to neutral B mesons. Using the global likelihood tool smelli, the authors found that the parameter space not excluded by the LHC is generally compatible with the Z pole and low-energy flavour observables, with one notable exception: the mass difference in the B_s mixing system, which can be in tension at up to three standard deviations depending on the relative sign of the Yukawa couplings. That tension could partially negate the fit improvement gained from explaining the non-leptonic anomalies, adding yet another obstacle for would-be model-builders.

The broader message is that the b to c anti-u q puzzle has grown more, not less, mysterious. The anomalies persist in channels where the theory is cleanest, and the new physics explanations that fit the flavour data most naturally predict collider signals that simply are not there. The authors conclude that these non-leptonic discrepancies will remain among the most puzzling deviations from the Standard Model for the foreseeable future, resolvable only in finely tuned scenarios that combine multiple Higgs doublets with unexpectedly large QCD power corrections. For experimentalists, the message is equally clear: the dijet and top-pair resonance searches at the LHC, often overshadowed by direct discovery channels, are doing quiet but decisive work in constraining the space of possible new physics, and future improvements in their systematics may ultimately settle whether the B meson anomaly is a window into new particles or simply a reminder that the strong force still holds secrets of its own.

Subject of Research: Non-leptonic B meson decay anomalies and constraints on new physics models from LHC collider searches

Article Title: New insights into the (b\rightarrow c \bar{u}q) puzzle through Top–Bottom synergies

Article References: Araz, J. Y., Englert, C., Kirk, M., & Tetlalmatzi-Xolocotzi, G. (2026). New insights into the $$b\rightarrow c \bar{u}q$$ puzzle through Top–Bottom synergies. The European Physical Journal C, 86(9), Article 1045. https://doi.org/10.1140/epjc/s10052-026-16297-5

Image Credits: AI Generated

DOI: 10.1140/epjc/s10052-026-16297-5

Keywords: B meson decays, flavour physics, QCD factorisation, two-Higgs-doublet model, LHC, dijet searches, top quark, new physics, Standard Model, power corrections, collider constraints, particle physics

The appeal of K+ → π+ ν ν̄ lies in its extraordinary cleanliness. Within the Standard Model the decay proceeds only through highly suppressed flavour-changing neutral-current processes, in which a strange quark converts into a down quark without altering its electric charge. The GIM mechanism, an interference effect among virtual quarks, suppresses the rate to roughly one part in ten billion. Unlike many other rare decays, the theoretical uncertainty is remarkably small, well under control thanks to decades of work on the electroweak corrections that dominate the amplitude. That combination of rarity and theoretical purity makes the branching ratio a precision probe of flavour violation among the first two quark generations, a sector where new heavy particles could otherwise leave faint but detectable fingerprints.

Allwicher and Bordone frame their analysis within the Standard Model Effective Field Theory, asking what the NA62 result implies under different assumptions about how new physics might couple to quarks and leptons. The first scenario they examine posits that new physics modifies the couplings of the Z boson to pairs of down-type quarks. A flavour-changing Z coupling of this kind would feed directly into rare decays at tree level, affecting both dineutrino channels such as K → π ν ν̄ and B → K ν ν̄ and the charged-lepton channel Bs → μ+ μ−. The relative impact on each process is governed by the flavour structure of the modified couplings, while the lepton couplings retain their Standard Model universality, making the correlation between observables especially transparent.

The authors test two competing flavour hypotheses within this scenario. Under Minimal Flavour Violation, new physics respects the CKM pattern of the Standard Model, and right-handed couplings are further suppressed by light-quark masses. In that case Bs → μ+ μ−, measured by ATLAS, CMS and LHCb with a combined uncertainty of roughly eight percent, remains the most constraining observable, and the kaon decay adds comparatively little. Partial Compositeness, inspired by composite Higgs and warped extra-dimension models, behaves very differently. There, the usual mass suppression of right-handed couplings is partially offset by inverse CKM factors, and kaon decays become strikingly sensitive. The analysis reveals a double solution in this case: one compatible with the Standard Model, and a second in which a new-physics contribution twice the size but opposite in sign cancels the Standard Model amplitude, leaving the decay rate unchanged. The newly measured B+ → K+ ν ν̄ branching fraction, recently observed by Belle II at a rate mildly above the Standard Model, can help discriminate between the two solutions.

The second scenario extends the analysis beyond neutral-current processes into semileptonic interactions. Here the authors work within a U(2)^5 flavour symmetry, a framework in which new physics couples predominantly to third-generation fermions, with small breaking terms connecting to the lighter families through CKM-suppressed spurions. This choice is motivated by the current experimental landscape, in which several tensions involving third-generation particles, including the R D(*) ratios of B decays into tau leptons, persist and are naturally accommodated in such a setup. The framework is governed by only four independent parameters, whose Wilson coefficients are constrained by a global fit spanning high-momentum Drell–Yan searches at the LHC, electroweak precision observables, lepton-flavour universality tests in tau decays, the semileptonic B anomalies, B → K ν ν̄ data, and the new kaon measurement itself.

The global fit produces a striking picture of correlated predictions. The scalar operator considered in the framework is tightly bounded by high-momentum searches and found consistent with zero, but the vector operators remain viable. Notably, the new NA62 measurement, with its substantially reduced uncertainty, dramatically narrows the region in which the kaon and B-meson dineutrino observables can be simultaneously satisfied. A particularly interesting branch of the fit corresponds to a large new-physics contribution that nearly cancels the Standard Model amplitude in K+ → π+ ν ν̄, producing an apparently SM-like branching ratio while permitting sizeable effects elsewhere. Upcoming NA62 precision at the fifteen percent level would severely test this cancellation, and the analysis shows how the remaining allowed region would shrink correspondingly.

The most tantalizing prediction concerns K_L → π^0 ν ν̄, the neutral partner mode that has never been observed. In the semileptonic third-generation scenario, the charged and neutral kaon modes respond differently to the underlying new-physics coefficient, and the fit predicts a characteristic hierarchy. Within the preferred region, the branching ratio of the neutral mode is expected to be enhanced relative to the Standard Model more strongly than the charged mode, with a ratio of roughly 1.5 between the two normalized enhancements. All predictions remain safely within the Grossman–Nir bound, the model-independent ceiling derived from the charged mode. The projected sensitivities of NA62 and the KOTO-II experiment at J-PARC, the latter targeting twenty-five percent precision, would put this correlation to a direct test, and together with Belle II’s projected eight percent precision on B+ → K+ ν ν̄ would provide a tripartite check of the entire framework.

The two scenarios also translate into very different statements about the energy scale of whatever new physics might be responsible. For modified Z couplings, the effective scale of the new interaction must exceed roughly eight teraelectronvolts, a value common to both flavour hypotheses because the dominant constraint acts on left-handed couplings. Although this scale sounds dauntingly high, the tree-level nature of the couplings means the high-luminosity LHC programme can still access the relevant phenomena directly. In the semileptonic third-generation scenario, by contrast, the effective scale sits near 1.8 teraelectronvolts, far closer to energies the LHC already explores, and the authors show that adding further operators would not qualitatively alter this conclusion because the new parameters enter largely independently of the fitted sector.

What emerges from the study is a vision of precision flavour physics as a connected network rather than a collection of isolated measurements. In the modified-Z scenario under Minimal Flavour Violation, an enhancement in the charged kaon mode is directly tied to an enhancement in B+ → K+ ν ν̄, and the authors further show that B → K* ν ν̄ responds differently to right-handed couplings than its charged counterpart, so measuring both B modes separately sharpens the constraints. Under Partial Compositeness the kaon measurement itself becomes the decisive observable, capable of resolving ambiguities that B_s → μ+ μ− alone cannot. In the semileptonic scenario, the kaon and B dineutrino branching ratios become coupled predictions of a single four-parameter framework, meaning that future measurements of any one of them will stress-test the whole edifice.

The timing of this convergence is no accident. The NA62 result, with a relative uncertainty below twenty percent, brings kaon decays into an era where they can genuinely compete with and complement B-factory and LHC measurements. Even though the current central values agree with the Standard Model, the study demonstrates that agreement is not the same as closure: under motivated flavour hypotheses, sizeable new physics can masquerade as a null result in one channel while manifesting openly in another. The coming generation of measurements, from NA62’s final precision through KOTO-II’s assault on the neutral kaon mode to Belle II’s dineutrino programme, will convert these theoretical correlations into concrete verdicts. If the patterns predicted by either scenario hold, particle physicists may finally glimpse the flavour structure of physics beyond the Standard Model; if they fail, entire classes of models will be swept away by the quietest decays in nature.

Subject of Research: Theoretical implications of the rare kaon decay K+ → π+ ν ν̄ for constraining new physics in B meson decays

Article Title: Implications of (K\rightarrow \pi \nu \bar{\nu }) for new physics in B decays

Article References: Allwicher, L., & Bordone, M. (2026). Implications of $$K\rightarrow \pi \nu \bar{\nu }$$ for new physics in B decays. The European Physical Journal C, 86(9), Article 1063. https://doi.org/10.1140/epjc/s10052-026-16313-8

Image Credits: AI Generated

DOI: 10.1140/epjc/s10052-026-16313-8

Keywords: kaon decay, NA62, flavour physics, new physics, B meson decays, Standard Model, effective field theory, Belle II, KOTO-II, rare decays, Z couplings, U(2) flavour symmetry