A self-consistent framework of topological amplitude and its SU(N) decomposition

Abstract

We propose a systematic theoretical framework for the topological amplitudes of the heavy meson decays and their SU(N) decomposition. In the framework, the topologies are expressed in invariant tensors and classified into tree- and penguin-operator-induced diagrams according to which four-quark operators, tree or penguin, being inserted into their effective weak vertexes. The number of possible topologies contributing to one type of decay can be counted by permutations and combinations. The Wigner-Eckhart theorem ensures the topological amplitudes under flavor symmetry are the same for different decay channels. By decomposing the four-quark operators into irreducible representations of SU(N) group, one can get the SU(N) irreducible amplitudes. Taking the D → PP decay (P denoting a pseudoscalar meson) with SU(3)F symmetry as an example, we present our framework in detail. The linear correlation of topologies in the SU(3)F limit is clarified in group theory. It is found there are only nine independent topologies in all tree- and penguin-operator-induced diagrams contributing to the D → PP decays in the Standard Model. If a large quark-loop diagram, named TLP, is assumed, the large ∆ACP and the very different D0→ K+K− and D0→ π+π− branching fractions can be explained with a normal U-spin breaking. Moreover, our framework provides a simple way to analyze the SU(N) breaking effects. The linear SU(3)F breaking and the high order U-spin breaking in charm decays are re-investigated in our framework, which are consistent with literature. Analogous to the degeneracy and splitting of energy levels, we propose the concepts of degeneracy and splitting of topologies to describe the flavor symmetry breaking effects in decay. As applications, we analyze the strange-less D decays in SU(3)F symmetry breaking into Isospin symmetry and the charm-less B decays in SU(4)F symmetry breaking into SU(3)F symmetry.

Mixing and $C\!P$ violation in charm decays at LHCb

“…The measurement of ΔA 𝐶𝑃 ≡ A 𝐶𝑃 (𝐷 0 → 𝐾 + 𝐾 − ) − A 𝐶𝑃 (𝐷 0 → 𝜋 + 𝜋 − ) with the full data sample collected by the LHCb detector led to the first observation of 𝐶𝑃 violation in the decay of charm hadrons [27]. The result challenges perturbative estimates of ΔA 𝐶𝑃 [25,28] and therefore prompted a renewed interest of the theory community in the field, sparking a discussion whether the measured value is consistent with the SM or if it is a sign of new physics [29][30][31][32][33][34][35][36][37][38][39]. Additional measurements of 𝐶𝑃 violation in the charm sector are thus crucial to clarify the picture and solve open theoretical puzzles.…”

A Review of $C\!P$ Violation Measurements in Charm at LHCb

“…) with the full data sample collected by the LHCb detector led to the first observation of CP violation in the decay of charm hadrons [44]. The result prompted a renewed interest of the theory community in the field, sparkling a discussion whether the signal is consistent with the Standard Model or if it is a sign of new physics [45][46][47][48][49][50][51][52][53][54][55]. Additional investigations are therefore crucial to clarify the picture and solve open theoretical puzzles.…”