Global Bayesian Analysis of new physics in b to s μμ transitions after Moriond-2019
Pith reviewed 2026-05-25 19:46 UTC · model grok-4.3
The pith
Bayesian global fit to b to s mu mu data after 2019 measurements updates credibility regions for new physics operators and compares models via Bayes factors.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
A Bayesian global fit to all available b to s ll observables, including the post-Moriond-2019 R_K, R_K*, and R_K*+ measurements, yields updated 68% and 95.4% credibility regions for the Wilson coefficients in several new-physics scenarios; pairwise Bayes factors identify the relative support for each scenario, while two classes of ultraviolet models (heavy Z' and scalar leptoquarks) are shown to furnish viable high-scale completions with explicit predictions for their couplings and masses.
What carries the argument
Bayesian global fit of effective operators for b to s mu mu transitions, with marginalization over nuisance parameters to obtain posterior credibility regions and direct computation of Bayes factors between pairs of models.
If this is right
- The 68% and 95.4% credibility regions for the new-physics Wilson coefficients are tightened by the inclusion of the 2019 data.
- Pairwise Bayes factors rank the relative viability of different operator combinations on the common data set.
- Explicit mass and coupling predictions are obtained for the Z' boson in vector-like fermion models.
- Explicit mass and coupling predictions are obtained for scalar leptoquark models.
Where Pith is reading between the lines
- The preferred operator patterns could be tested by measuring additional angular observables in the same decays.
- The derived mass ranges for the Z' or leptoquarks can be confronted with direct searches at the LHC.
- If the current hierarchy of Bayes factors persists, it would favor flavor structures that suppress electron modes relative to muons.
Load-bearing premise
All relevant new physics effects are captured by the finite set of effective operators retained in the fit, with negligible contributions from any operators or scales omitted from the analysis.
What would settle it
A future high-precision measurement of any R_K-like ratio or angular observable that lies outside the 95.4% credibility region obtained for every scanned scenario would falsify the fit results.
Figures
read the original abstract
The recent measurement of $R_K$ at LHCb continues to support the hint of violation of lepton flavor universality. We perform a global fit for new physics in semileptonic $b\to s$ transitions using all the relevant data with a Bayesian analysis technique. We include new measurements of $R_K$ at LHCb and new determinations of $R_{K^*}$ and $R_{K^{*+}}$ at Belle. We perform the scan for various NP scenarios and infer the 68\% and 95.4\% credibility regions of the marginalized posterior probability density for all scenarios. We also compare the models in pairs by calculating the Bayes factor given a common data set. A few well-known BSM models are analyzed that can provide a high energy framework for the EFT analysis. These include the exchange of a heavy $Z^{'}$ boson in models with heavy vector-like fermions and a scalar field, and a model with scalar leptoquarks. We provide predictions for the BSM couplings and expected mass values.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper performs a global Bayesian fit to new physics in b→sμμ transitions incorporating the post-Moriond-2019 LHCb R_K measurement and Belle R_K* and R_K*+ results. It scans multiple NP scenarios, extracts 68% and 95.4% credibility regions on the marginalized posteriors for the Wilson coefficients, computes pairwise Bayes factors on a common dataset, and matches a subset of scenarios to UV models (heavy Z' with vector-like fermions, scalar leptoquarks) to predict couplings and masses.
Significance. If the results hold, the work supplies an updated, statistically coherent snapshot of the b→sℓℓ anomalies with quantitative model discrimination via Bayes factors and direct links to concrete BSM realizations. The inclusion of the newest R_K and R_K* data and the use of standard Bayesian outputs (credibility regions, Bayes factors) are clear strengths.
major comments (1)
- [EFT setup and fit definition] The central results (credibility regions and Bayes-factor rankings) rest on the assumption that NP contributions are exhausted by the specific set of effective operators retained in the fit. The manuscript does not quantify the effect of enlarging the operator basis (e.g., additional right-handed currents or four-fermion operators outside the baseline set), leaving open the possibility that the reported regions and model preferences would shift if such contributions are present.
minor comments (2)
- Clarify the exact list of observables and their correlations used in the likelihood; a table summarizing the data set would improve reproducibility.
- State the prior ranges and functional forms adopted for the Wilson coefficients explicitly, including any correlations imposed between real and imaginary parts.
Simulated Author's Rebuttal
We thank the referee for the positive assessment of our work and for the detailed comment on the EFT setup. We respond to the point raised below.
read point-by-point responses
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Referee: [EFT setup and fit definition] The central results (credibility regions and Bayes-factor rankings) rest on the assumption that NP contributions are exhausted by the specific set of effective operators retained in the fit. The manuscript does not quantify the effect of enlarging the operator basis (e.g., additional right-handed currents or four-fermion operators outside the baseline set), leaving open the possibility that the reported regions and model preferences would shift if such contributions are present.
Authors: Our analysis is performed within the standard basis of dimension-six operators relevant to b→sμμ transitions that is conventionally adopted in global fits to these anomalies. This basis is chosen because it captures the leading effects needed to accommodate the data while remaining consistent with existing constraints from other observables. The various NP scenarios we scan, as well as the matching to UV models (Z' and scalar leptoquarks), are defined within this framework. We agree that a larger operator set could in principle modify the posteriors and Bayes factors; however, such an extension would introduce additional free parameters whose effects cannot be robustly constrained by the current dataset alone and would require a substantially more involved analysis. The reported credibility regions and model rankings are therefore conditional on the adopted operator basis, which is the standard practice in the literature for this class of studies. revision: no
Circularity Check
No significant circularity; analysis is a direct Bayesian fit to external data
full rationale
The paper conducts a standard global Bayesian fit of effective operator coefficients to experimental observables in b→sμμ transitions, deriving posterior credibility regions and Bayes factors from the data likelihood. No quoted steps show self-definitional relations, fitted inputs relabeled as predictions, or load-bearing self-citations that reduce the central results to the inputs by construction. The BSM model matching and mass predictions follow from the EFT posteriors matched to UV completions, but remain externally constrained by the same data set. This is a self-contained statistical analysis against independent experimental inputs.
Axiom & Free-Parameter Ledger
free parameters (1)
- Wilson coefficients
axioms (1)
- domain assumption New physics effects are captured by dimension-6 operators in the b->sll effective Lagrangian
Reference graph
Works this paper leans on
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[1]
The red star marks the position of the best-fit point
is presented. The red star marks the position of the best-fit point. The gray solid (dashed) line shows the 1 σ (2σ) cred- ible region of the pdf corresponding to the data pre- LHCb Run 2. The associated best-fit point is also shown in gray. The new measurement ofRK, which is slightly higher than the previous measurement, brings the 2σ region closer to the ...
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[2]
Cµ 10, C′µ 9 , C′µ 10 and make the comparison between the marginalized pdf in the ( Cµ 9 , Cµ
(left) and ( Cµ 9 , C′µ 9 ) (right). Cµ 10, C′µ 9 , C′µ 10 and make the comparison between the marginalized pdf in the ( Cµ 9 , Cµ
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[3]
The large negative values of Cµ 9 are favored by the data with 4 parameters
plane for the scan with 2 input NP parameters, and the one with 4 NP parameters which is shown in the left of Figure 3. The large negative values of Cµ 9 are favored by the data with 4 parameters. In the middle of Figure 3, we show a comaprison between the marginalized pdf in the (Cµ 9 , C′µ 9 ). It can be seen that ample region of C′µ 9 ≤ 0 is allowed du...
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[4]
This suggests that NP with only muon sector can easily explain the present data
In the lower panel of Figure 4, a marginalized pdf for electron sector Wilson coefficients are presented which is consistent with zero at 2 σ. This suggests that NP with only muon sector can easily explain the present data. In Figure 5, we present the marginalized pdf for 8 pa- rameter scan in most relevant planes ( Cµ 9 , Cµ
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[5]
and (Cµ 9 ,C′µ 9 ) in the left and right panel. These marginal pdf are compared with 2 parameter scan and we find that these figures are almost same as Figure 3 which is expected as the NP wilson coefficients in the electron sector have limited impact on the data. We use Jeffrey’s scale to quickly assess the Bayes factor, which will point to which model is fav...
work page 2019
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78.3 4.4σ 135.4 1 .02 123.3 6.6 0 .2 5 .4 TABLE I: Evidence, pull from the SM, and chi-squared statistics for the best-fit points of the considered scenarios. Second row in each block correspond to the new data, while the first ones show the previous determinations. IV. MODEL DEPENDENT ANAL YSIS A. Heavy Z ′ The most generic Lagrangian, parametrizing LFUV c...
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Second row in each correspond to the new data, while the first ones show the previous determinations
−1.05 0.13 0.10 −0.38 −2.18 −0.07 −2.73 −1.34 TABLE II: Wilson coefficients at the best-fit points, as well as the values there of RK and RK∗. Second row in each correspond to the new data, while the first ones show the previous determinations. is required to generate ∆ sb L and ∆sb R . Thus, in this work we also consider the impact of the new LHCb and Belle ...
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