Bridging the Gap: Hadronic and Partonic Views of Particle Decay

Author: Denis Avetisyan


New research reconciles theoretical calculations of rare particle decays, showing how hadronic effects can be consistently incorporated into established analytic frameworks.

The complex-valued trajectory of <span class="katex-eq" data-katex-display="false">s + s_{+}\</span> reveals the parameter-dependent thresholds for partonic and hadronic transitions-specifically, <span class="katex-eq" data-katex-display="false">s_{\text{th}} = 4m_{c}^{2}</span> and <span class="katex-eq" data-katex-display="false">s_{\text{th}} = 4M_{D}^{2}</span>-with physical crossing points occurring at <span class="katex-eq" data-katex-display="false">\xi = 1</span> for <span class="katex-eq" data-katex-display="false">b \to s</span> (<span class="katex-eq" data-katex-display="false">m_{1} = m_{c} + m_{s}</span>), <span class="katex-eq" data-katex-display="false">\xi = 2.04</span> for <span class="katex-eq" data-katex-display="false">B \to K</span> (<span class="katex-eq" data-katex-display="false">m_{1} = M_{D^{<i>}}\_{s}</span>), and <span class="katex-eq" data-katex-display="false">\xi = \{3.69, 8.62\}</span> for <span class="katex-eq" data-katex-display="false">B \to K^{</i>}\</span> (<span class="katex-eq" data-katex-display="false">m_{1} = \{M_{D^{*}}\_{s}, M_{D\_{s}}\}</span>), as determined by analysis utilizing mass values from Navaset al. (2024).
The complex-valued trajectory of s + s_{+}\ reveals the parameter-dependent thresholds for partonic and hadronic transitions-specifically, s_{\text{th}} = 4m_{c}^{2} and s_{\text{th}} = 4M_{D}^{2}-with physical crossing points occurring at \xi = 1 for b \to s (m_{1} = m_{c} + m_{s}), \xi = 2.04 for B \to K (m_{1} = M_{D^{<i>}}\_{s}), and \xi = \{3.69, 8.62\} for B \to K^{</i>}\ (m_{1} = \{M_{D^{*}}\_{s}, M_{D\_{s}}\}), as determined by analysis utilizing mass values from Navaset al. (2024).

This review demonstrates the consistency of perturbative and dispersive techniques in analyzing b→sℓℓ transitions, resolving concerns about missing anomalous hadronic contributions.

Discrepancies in rare $B$-meson decays offer tantalizing hints of physics beyond the Standard Model, yet robust interpretations require careful control over theoretical uncertainties. This paper, ‘Reconciling hadronic and partonic analyticity in $b\to s\ell\ell$ transitions’, addresses this challenge by investigating the analytic structure of nonlocal form factors relevant to b\to s\ell\ell transitions. We demonstrate that calculations based on perturbative expansions consistently match those derived from dispersive techniques, even in the presence of anomalous thresholds, thereby validating their use in parameter regions where a perturbative approach is justified. Does this reconciliation pave the way for more precise Standard Model tests and a definitive search for new physics in these sensitive decays?


Unveiling New Physics: Anomalies in B-Meson Decay

Recent investigations into the decay of B mesons into strange particles and pairs of leptons – specifically, b \rightarrow s\ell\ell transitions – are challenging the established framework of the Standard Model of particle physics. Experiments at facilities like the Large Hadron Collider beauty experiment (LHCb) have detected a statistically significant discrepancy between observed decay rates and the precise predictions made by the Standard Model. This isn’t a definitive discovery of new particles, but rather a compelling indication that additional, yet unknown, forces or particles may be influencing these decays. The observed anomalies primarily manifest as an unexpected distribution of lepton momentum, suggesting the involvement of particles that interact with both b quarks and leptons. Consequently, physicists are actively pursuing a variety of theoretical models – including those involving leptoquarks and Z’ bosons – and designing new experiments to confirm or refute these intriguing hints of physics beyond the Standard Model.

Unraveling the mysteries surrounding potential new physics requires an unprecedented level of precision in theoretical calculations. The observed anomalies in b \rightarrow s \ell \ell transitions, while suggestive of physics beyond the Standard Model, exist alongside substantial, and often complex, Standard Model backgrounds. Distinguishing a genuine signal of new particles or interactions from these backgrounds isn’t simply a matter of observing a difference; it demands calculations that can predict the Standard Model contribution to an extraordinary degree of accuracy. These calculations involve intricate quantum loop effects and necessitate advanced techniques to handle the inherent uncertainties, effectively establishing a benchmark against which any deviation – potentially hinting at new physics – can be rigorously assessed. Without this precise theoretical framework, even a significant observed anomaly could be misinterpreted, obscuring the path toward a more complete understanding of the universe.

Partonic diagrams <span class="katex-eq" data-katex-display="false"> (a)-(e) </span> and their corresponding triangle interpretations are presented with normal thresholds and anomalous branch points calculated for <span class="katex-eq" data-katex-display="false"> m_{c}^{2}/m_{b}^{2} = 0.1 </span> and <span class="katex-eq" data-katex-display="false"> m_{s} = 0 </span>, highlighting the analytic structure of the spectral function.
Partonic diagrams (a)-(e) and their corresponding triangle interpretations are presented with normal thresholds and anomalous branch points calculated for m_{c}^{2}/m_{b}^{2} = 0.1 and m_{s} = 0 , highlighting the analytic structure of the spectral function.

Nonlocal Form Factors and the Charm Loop Challenge

Nonlocal form factors arise in the theoretical description of b \rightarrow s \ell \ell decays due to the long-distance contributions from strong interactions. These form factors parameterize the effects of virtual particles exchanged between the decaying b-quark and the final state leptons, extending beyond the simplified point-like interaction assumptions. Accurate determination of these form factors is essential because they introduce significant systematic uncertainties in predictions for observables like the lepton flavor universality ratio R_{K} and angular distributions. Calculations typically involve operator product expansion (OPE) and subsequent matching to the full theory, requiring careful renormalization and handling of infrared divergences. The precision demanded by current and future experiments, such as LHCb, necessitates calculations at next-to-next-leading order (NNLO) or even higher, coupled with robust non-perturbative input for parameters like the \Lambda_{QCD} scale.

Charm loops, arising from virtual charm quarks in the decay amplitude of b \rightarrow s \ell \ell processes, represent a significant source of theoretical uncertainty in the determination of form factors. These loops contribute to the calculation of non-local matrix elements and introduce long-distance effects that can, if not accurately modeled, obscure potential signals of Beyond the Standard Model (BSM) physics. Specifically, the interference between the Standard Model amplitudes involving charm loops and hypothetical BSM contributions can mimic new physics signatures in observables such as the P_5' polarization fraction or the lepton flavor universality ratios. Precise control of these loop-induced effects requires the use of Operator Product Expansion (OPE) and careful renormalization procedures to ensure accurate predictions and reliable searches for new physics.

Precise determination of form factor analytic properties is essential for new physics searches in b \rightarrow s \ell \ell decays because these form factors appear in the amplitude as rational functions with potential poles and singularities. These singularities can, if not properly accounted for, either mask genuine new physics signals or, conversely, create spurious signals mimicking physics beyond the Standard Model. Specifically, a detailed understanding of the kinematic regions where the form factors are well-behaved – and the locations of any singularities – is required to define control regions in experimental analyses, allowing for accurate estimations of background contributions and reliable extraction of new physics parameters. Accurate modeling of the form factor’s analytic structure therefore directly impacts the sensitivity and interpretability of searches for beyond the Standard Model phenomena.

Two-loop partonic diagrams for <span class="katex-eq" data-katex-display="false">b \to s \gamma^*</span> decays, featuring charm loops and utilizing the conventions of Asatrian et al. (2020), illustrate the coupling of the electromagnetic current to either <span class="katex-eq" data-katex-display="false">b</span> or <span class="katex-eq" data-katex-display="false">c</span> quarks via the effective operators <span class="katex-eq" data-katex-display="false">\mathcal{O}_{1,2}</span>, with diagrams exhibiting current insertion at the <span class="katex-eq" data-katex-display="false">b</span> or <span class="katex-eq" data-katex-display="false">s</span> quark dominating.
Two-loop partonic diagrams for b \to s \gamma^* decays, featuring charm loops and utilizing the conventions of Asatrian et al. (2020), illustrate the coupling of the electromagnetic current to either b or c quarks via the effective operators \mathcal{O}_{1,2}, with diagrams exhibiting current insertion at the b or s quark dominating.

Reconstructing Form Factors: A Dispersive Approach

A dispersive approach to determining nonlocal form factors leverages the principles of analyticity – specifically, the ability to reconstruct a function from its known discontinuities – and combines this with available experimental data. This methodology circumvents the need for specific models by directly relating the form factor to measurable quantities via dispersion relations. By accurately modeling the analytic structure, including contributions from singularities and cuts, the dispersive approach provides a model-independent constraint on the form factor’s value and functional behavior, offering a robust and precise determination that is less susceptible to systematic uncertainties arising from assumptions about the underlying dynamics.

Form factor reconstruction via the dispersive approach centers on calculating the discontinuities of the form factor, which are directly related to the imaginary part of the scattering amplitude. These discontinuities are computed using triangle diagrams, a Feynman diagram topology representing the exchange of a virtual particle, and spectral functions. The spectral function encapsulates the contributions from all possible intermediate states, effectively modeling the left-hand cut in the dispersion integral. By accurately determining these discontinuities and integrating accordingly, the complete form factor can be reconstructed, providing a model-independent determination of relevant observables.

The spectral function, a key component in dispersive analyses of form factors, directly parameterizes the left-hand cut and is fundamentally determined by the contributions of intermediate hadronic states. Specifically, the presence of resonances and thresholds, such as those originating from the D meson and its excitations, significantly influence the shape and magnitude of the spectral function. Accurate modeling of these intermediate state contributions is essential for a precise determination of the form factor, as the spectral function effectively encodes information about the underlying strong interaction dynamics that govern the decay process. The weighting of each intermediate state is dictated by its coupling to the initial and final states and its propagator, which is determined by its mass and width.

Two-loop evaluations within the dispersive approach are essential for achieving theoretical precision by incorporating higher-order Quantum Chromodynamics (QCD) corrections to the form factor calculations. These calculations extend beyond the leading-order approximations, accounting for contributions from virtual particles and complex interactions that influence the observed physical quantities. Our results demonstrate the internal consistency of these two-loop computations, evidenced by the convergence of perturbative series and agreement between different calculation methods. This validation confirms the reliability of the dispersive approach as a means of reconstructing form factors and provides a robust framework for extracting precise values for relevant parameters in particle physics.

Deviations between results derived from the dispersion relation and those from a 22-loop calculation remain small across a range of <span class="katex-eq" data-katex-display="false">s</span> values, except where instabilities arise in the EOS software at high <span class="katex-eq" data-katex-display="false">s</span>, indicating a limitation of the implementation.
Deviations between results derived from the dispersion relation and those from a 22-loop calculation remain small across a range of s values, except where instabilities arise in the EOS software at high s, indicating a limitation of the implementation.

The Role of Analytic Structure and Viriality in Precision Calculations

The analytic structure of form factors, which describe the amplitude of particle interactions, is directly influenced by the spacelike virtuality – the off-shell momentum transfer in a scattering process. As the virtuality increases, the form factors can exhibit singularities, specifically poles and branch points, arising from the underlying dynamics of the interacting particles. These singularities manifest as divergences in the mathematical expressions for the form factors and necessitate careful handling through techniques like analytic continuation and appropriate choice of integration contours. Failure to address these singularities correctly can lead to inaccurate predictions for scattering amplitudes and observable physical quantities. The location and nature of these singularities provide valuable information about the internal structure and composition of the particles involved, and their precise determination is crucial for maintaining the consistency of theoretical calculations.

Anomalous thresholds within the analytic structure of form factors introduce distortions that impede accurate dispersive reconstruction. These thresholds, deviating from standard behavior, manifest as irregularities in the integral used to derive form factors from experimental data. Consequently, the standard application of dispersion relations-a technique relying on the analytic properties of the integrand-becomes problematic, leading to inaccuracies or divergences in the reconstructed form factor. Addressing these distortions necessitates careful consideration of the threshold behavior, potentially requiring modified integration techniques or the implementation of subtraction procedures to isolate and remove the anomalous contributions before applying the dispersive reconstruction process.

Dispersion relations, integral equations relating a particle’s scattering amplitude to its response function, are susceptible to logarithmic singularities arising from the integral’s behavior at the boundaries or due to the presence of branch points. These singularities, often appearing as \ln(s) terms where s represents the Mandelstam variable, invalidate the direct application of the dispersion relation and necessitate the implementation of regularization techniques. Common approaches include dimensional regularization or the introduction of a cutoff to control the integral’s high-energy behavior, effectively modifying the integrand to remove the singularity while preserving the underlying physics. Proper regularization is crucial for obtaining physically meaningful and finite results when reconstructing form factors from dispersive analyses.

Analysis demonstrates the calculated analytic structure aligns with established dispersion relations, thereby validating the perturbative calculations utilized in the form factor reconstruction. This consistency is crucial as it allows for the integration of these results with hadronic models, enabling combined analyses that leverage the strengths of both perturbative and non-perturbative approaches. Specifically, the established analytic structure provides a robust framework for extrapolating results beyond the perturbative regime and for incorporating the complexities of strong interaction dynamics described by hadronic models. The validated framework allows for more accurate predictions and a deeper understanding of the underlying physics.

Comparison of the real and imaginary parts of the form factors for diagrams (b) and (d) demonstrates strong agreement between our dispersion relation results and the exact 22-loop calculations from Asatrian et al. (2020).
Comparison of the real and imaginary parts of the form factors for diagrams (b) and (d) demonstrates strong agreement between our dispersion relation results and the exact 22-loop calculations from Asatrian et al. (2020).

Towards Precision Phenomenology and New Physics Discovery

Precise calculations of b \rightarrow s \ell \ell decays are crucial for probing the Standard Model and searching for new physics, and a powerful method for achieving this relies on combining the dispersive approach with a detailed understanding of the analytic structure of the relevant amplitudes. This technique circumvents the need for potentially unreliable assumptions about the high-energy behavior of these decays by reconstructing the full theoretical prediction from experimental data and theoretical constraints. By carefully analyzing the singularities and branch points in the complex momentum plane, physicists can determine the contributions from various physical processes, leading to predictions that are demonstrably more robust and accurate than those obtained through traditional perturbative methods. This rigorous framework allows for a stringent test of the Standard Model’s predictions and provides a sensitive means of detecting subtle deviations that could signal the presence of new particles or interactions.

The precision offered by this dispersive approach enables exceptionally rigorous examinations of the Standard Model’s predictions regarding b \rightarrow s \ell \ell decays. Subtle deviations from established theoretical values, even those previously masked by uncertainties, become potentially discernible, opening a pathway to identify signals indicative of new physics. This sensitivity stems from the framework’s ability to isolate and amplify the effects of hypothetical particles or interactions beyond those currently described, effectively acting as a powerful probe for physics residing beyond the Standard Model. Consequently, the detailed analysis of these decays offers a compelling means to both validate the existing framework and, crucially, to uncover evidence of fundamental forces and particles yet to be observed.

The research detailed establishes a robust theoretical groundwork intended to catalyze further exploration within the field of particle physics. By meticulously outlining a dispersive approach to analyzing b \rightarrow s \ell \ell decays, the framework not only offers precise predictions but also facilitates the creation of increasingly sophisticated analytical techniques. This foundation empowers future studies to delve deeper into the intricacies of the Standard Model and to more effectively search for subtle deviations indicative of new physics. Consequently, the methodology presented promises to accelerate progress in understanding the fundamental constituents of the universe and the forces governing their interactions, paving the way for advancements beyond current theoretical limits.

The pursuit of precision in particle physics, exemplified by investigations into b→sℓℓ decays, directly addresses foundational questions about the universe’s governing laws. These calculations, rigorously validated through consistency with both dispersion relations and established hadronic models, aren’t merely tests of the Standard Model; they actively probe for deviations indicative of new physics. Any discrepancy, however subtle, could reveal the presence of particles or interactions beyond our current understanding, potentially reshaping the landscape of fundamental physics. This methodical approach – refining theoretical predictions and comparing them to experimental data – offers a powerful pathway to unveil the underlying structure of reality and expand the horizons of established physical laws, ultimately pushing the boundaries of human knowledge regarding the universe’s most basic constituents and forces.

Comparison of the real and imaginary parts of the finite-frequency (FF) response for two diagrams reveals strong agreement between our dispersion relation results and the exact <span class="katex-eq" data-katex-display="false">\mathcal{O}(22</span>-loop) calculations from Asatrian et al. (2020).
Comparison of the real and imaginary parts of the finite-frequency (FF) response for two diagrams reveals strong agreement between our dispersion relation results and the exact \mathcal{O}(22-loop) calculations from Asatrian et al. (2020).

The pursuit of reconciling hadronic and partonic analyticity, as detailed in the study of $b\to s\ell\ell$ transitions, demands a rigorous examination of underlying structures. It isn’t merely about calculating observable effects, but understanding how those effects emerge from the interplay of complex systems. This echoes Richard Feynman’s sentiment: “The first principle is that you must not fool yourself – and you are the easiest person to fool.” The work carefully navigates potential self-deceptions in perturbative calculations by demonstrating consistency with dispersive techniques, ensuring the observed results aren’t artifacts of the method itself. Such precision reflects a commitment to unveiling the genuine analytic structure, rather than being misled by superficial appearances, and reveals how structure dictates behavior in these particle transitions.

The Road Ahead

The insistence on analytic consistency, as demonstrated in this work, is less a resolution and more a sharpening of the questions. One does not simply ‘fix’ the low-energy description of $b \to s\ell\ell$ transitions; rather, one must understand the entire circulation of information between the perturbative and hadronic realms. To believe a calculation is complete because it matches a particular analytic structure is akin to treating a symptom while ignoring the patient. The established framework, while internally consistent, remains vulnerable to subtleties in the operator product expansion – the implicit assumptions about the scale at which hadronic effects become negligible.

Future progress will inevitably require a deeper engagement with the limitations of form factor parameterizations. The search for anomalous thresholds, while yielding negative results to date, should not be abandoned, but refined with a more holistic view of the underlying dynamics. The true test will not be simply to reproduce existing results, but to predict novel observables sensitive to the interplay between short- and long-distance effects – signals that might otherwise be obscured by the very techniques employed to isolate them.

Ultimately, the pursuit of precision in this field demands a certain humility. One must acknowledge that the current theoretical edifice, elegant as it may be, is built upon a foundation of approximations. The persistence of anomalies, even in the face of increasingly sophisticated calculations, serves as a constant reminder that the complete picture remains elusive – and that the most interesting discoveries often lie just beyond the reach of our current understanding.


Original article: https://arxiv.org/pdf/2604.01284.pdf

Contact the author: https://www.linkedin.com/in/avetisyan/

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2026-04-05 21:10