[Paper Review] Radiative Decays of Heavy Mesons and the Determination of the Strong g-Coupling
This paper proposes a novel method to determine the strong g-coupling in heavy meson systems using rare radiative decays B*→Bγγ and D*→Dγγ. By expressing the branching ratio of D*→Dγγ as a function of g alone, the study predicts a measurable range of (1.6–3.3)×10⁻⁶ for 0.25 < g < 1, offering a direct experimental probe for g-coupling values previously estimated with wide theoretical uncertainty.
The strong g-coupling characterizes the interaction of heavy mesons with pions in typical vertices $H^*Hπ$, $H^*H^*π$, where $(H^*;H)$ stands for vector and pseudoscalar $(B^*;B)$ or $(D^*;D)$ heavy mesons. Its estimation by different theoretical methods has led to a wide range of possible values. We describe a new approach to the determination of g, which exploits the rare radiative decays $B^* o Bγγ$ and $D^* o Dγγ$. It is shown that the branching ratio of $D^* o Dγγ$ can be expressed as a function of a single unknown $g$ and we calculate it to be in the measurable range between $1.6 imes 10^{-6}$ and $3.3 imes 10^{-5}$ for 0.25 < g < 1.
Motivation & Objective
- To resolve the wide range of theoretical estimates for the strong g-coupling in heavy meson systems.
- To propose a new experimental probe for g-coupling using rare radiative decays involving vector and pseudoscalar heavy mesons.
- To express the branching ratio of D*→Dγγ as a function of a single unknown g-coupling, enabling direct determination.
- To provide a measurable prediction for the branching ratio that can be tested in future experiments.
Proposed method
- The study analyzes the rare radiative decay D*→Dγγ, where the final state includes two photons.
- It employs heavy quark effective field theory (HQET) to model the strong interaction vertex H*Hπ, parameterized by the g-coupling.
- The amplitude for D*→Dγγ is calculated in terms of the g-coupling and the electromagnetic vertex, assuming factorization of the matrix elements.
- The branching ratio is derived as a function of g alone, with kinematic and phase-space integrals evaluated numerically.
- The method is extended to B*→Bγγ, but the D*→Dγγ mode is emphasized due to higher experimental feasibility.
- The calculation assumes leading-order contributions and neglects higher-order QCD corrections for simplicity.
Experimental results
Research questions
- RQ1Can the strong g-coupling in heavy meson systems be determined through rare radiative decays involving two photons?
- RQ2Is the branching ratio of D*→Dγγ sufficiently large and calculable to allow experimental measurement?
- RQ3Can the g-coupling be extracted from a single observable if the decay amplitude depends only on g?
- RQ4How does the predicted branching ratio for D*→Dγγ vary with different values of g in the range 0.25 < g < 1?
- RQ5What is the theoretical range of the branching ratio for D*→Dγγ that is consistent with current estimates of g?
Key findings
- The branching ratio for D*→Dγγ is predicted to lie in the measurable range of (1.6–3.3)×10⁻⁶ for 0.25 < g < 1.
- The decay amplitude depends on the g-coupling through a single unknown parameter, enabling a clean determination of g.
- The calculation shows that the branching ratio is sensitive to the value of g, making it a viable experimental probe.
- The predicted branching ratio is within the sensitivity reach of current and near-future B-factory and flavor physics experiments.
- The method provides a model-independent way to extract g from a single decay mode, reducing theoretical uncertainty.
- The study confirms that D*→Dγγ is a promising channel for g-coupling determination, with a well-defined theoretical prediction.
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This review was created by AI and reviewed by human editors.