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Dao-Neng Gao

Publications and source records attributed to Dao-Neng Gao.

At least 19 recordsLinked to original sources

Improved analysis of rare $Z$-boson decays into a heavy vector quarkonium plus lepton pair

We improve the theoretical predictions for rare $Z$-boson decays, $Z\to V\ell^+\ell^-$ ($\ell=e$ or $μ$), where $V$ denotes a heavy vector quarkonium including $J/Ψ$, $Ψ(2S)$, and $Υ(nS)$ with $n=1,2,3$. These processes are thought to be dominated by the electromagnetic fragmentation transition, i.e., $Z\to γ^*\ell^+\ell^-$ followed by $γ^*\rightarrow V$. The present study includes all of the relevant tree-level Feynman diagrams, which contribute to these decays in the standard model. Our analysis shows that, for the charmonium final states, the fragmentation transition almost saturates the whole contribution and the other diagrams can be neglected; while for the bottomonium final states, the inclusion of other diagrams can increase their branching fractions by $4\%\sim 9\%$. Further investigation of the differential distributions, especially the angular distributions, indicates that forward-backward asymmetries for final leptons in these processes would be zero in the standard model. Therefore, in future experimental facilities with large number of $Z$-boson events accumulated, studies of these rare $Z$ decays may help both to test the standard model and to probe its interesting extensions.

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Rare $W$-boson decays into a vector meson and lepton pair

We have presented a theoretical study of exclusive rare $W$-boson decays, $W\to V\ell\barν_\ell$ with $V$ denoting a neutral vector meson and $\ell=e$ or $μ$, in the standard model. The leading-order contributions to these processes are given by $W\to γ^*\ell\barν_\ell$ with the subsequent $γ^*\to V$ transition. Branching fractions of these decay modes, for $V=ρ$, $ω$, $ϕ$, and $J/Ψ$, respectively, have been calculated and predicted around $10^{-6}\sim 10^{-7}$, which are surprisingly larger than those of two-body hadronic radiative decays $W^\pm\to M^\pm γ$ with $M$ denoting a pseudoscalar or vector meson. Thus it is expected that rare $W$ decays into a neutral vector meson plus lepton pair may be the promising channels in future experimental facilities with a large number of $W$-boson events produced.

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Note on rare $Z$-boson decays to double heavy quarkonia

Within the standard model, we have investigated rare $Z$-boson decays into double heavy quarkonia, $Z\to VV$ and $Z\to VP$ with $V$ denoting vector and $P$ denoting pseudoscalar quarkonia, respectively. It is assumed that the leading-order QCD diagrams would give the dominant contributions to these processes, and the corresponding branching fractions, for instance, ${\cal B}(Z\to J/ΨJ/Ψ)$ has been estimated to be around $10^{-13}$ in the literature. However, these decays could also happen through the electromagnetic transition $Z\to Vγ^*$ and $Z\to Pγ^*$, with the virtual photon transforming into $V$. Interestingly, the smallness of the vector quarkonium mass can give rise to a large factor $m_Z^2/m_V^2$, relative to the QCD contributions, which thus counteracts the suppression from the electromagnetic coupling. We systematically include these two types of contributions in our calculation to predict branching fractions for these decays. Particularly, due to the virtual photon effects, it is found that ${\cal B}(Z\to J/ΨJ/Ψ)$ will be significantly enhanced, which could be up to $10^{-10}$.

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Higgs boson decays into a pair of heavy vector quarkonia

Rare Higgs decays into a pair of heavy vector quarkonia, $h\to VV$ ($V=J/Ψ$, $Υ$ etc.), have been investigated in the standard model. Different from the past literature in which these decays are thought to be only dominated by the longitudinally polarized final states, we also include the transitions, which proceed through $h\to γ^*γ^*$/$h\to Vγ^*$, followed by $γ^*\to V$. The final vector quarkonia via these ways are dominantly transversely polarized. Our calculation however shows that these transitions could lead to significant contributions to the decay rate, especially for the charmonium final states. The total branching ratios of these processes are predicted to be around $10^{-10}$, far below the current experimental upper bounds. Hopefully, experimental studies of these very rare decays in future high-precision experimental facilities might be interesting both to test the standard model and to look for new physics scenarios.

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Exclusive rare Higgs decays into lepton pair and light mesons

Exclusive rare Higgs decays into lepton pair plus one light hadron, such as $h\to ρ^0(ω)\ell\bar{\ell}$, $h\to π^0\ell\bar{\ell}$, $h\to π^+ (K^+)\ell^-\barν_\ell$, and $h\to ρ^+(K^{*+})\ell^-\barν_\ell$, have been explored in the standard model. Decay amplitudes are dominantly from the Higgs couplings to gauge bosons and to charged leptons, and their branching ratios are predicted in the range of $10^{-8}\sim 10^{-5}$. We have also analyzed the differential dilepton invariant mass and angular distributions of $h\to ρ^0 \ell^+\ell^-$ decays. It will be challenging to search for these rare processes. Nevertheless, experimental studies of them, in particular, $h\to ρ^0\ell^+\ell^-$ with $\ell=e,μ$, might be interesting both to help deepen our understanding of the standard model and to probe new physics beyond the standard model in the future high-precision experiments.

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Impact on the decay rate of $B_s\to μ^+μ^-$ from the dispersive two-photon transition

We study the long-distance contribution to $B_s\toμ^+μ^-$ decay, which is generated by the two-photon intermediate state via $B_s\toγ^*γ^*\toμ^+μ^-$ transition. It is found that the dispersive two-photon amplitude can interfere with the dominant short-distance amplitude, which gives rise to new theoretical uncertainty in the branching ratio of $B_s\toμ^+μ^-$. Our analysis shows that, by taking into account present experimental constraints, this uncertainty could be up to the same order of magnitude as some theoretical uncertainties of ${\cal B}(B_s\toμ^+μ^-)$ given in the past literature. Future precise studies of the double radiative $B_s\toγγ$ decay, both experimentally and theoretically, may help to reduce the uncertainty. This novel effect has never been examined in $B_s\toμ^+μ^-$ decay.

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Note on invisible decays of light mesons

A search for the invisible decays of $ω$ and $ϕ$ mesons in $J/ψ\to ω(ϕ)η$ transitions has been performed by the BESIII Collaboration very recently. Inspired by this experimental study, we compute the lowest order contribution to branching ratios of ${\cal B}(V\to\barνν)$ with $V$ denoting $ρ,\;ω,\;ϕ$, as the standard model background to these invisible decays. Our predictions are far below the upper bounds given by the BESIII experiment. We also analyze the $J/ψ\to η(η^\prime)\barνν$ processes, and estimate their decay rates. Furthermore, the invisible decays of light pseudoscalar mesons $P$ including $π^0$, $η$, and $η^\prime$ are reexamined in the present note. It is shown that, due to the helicity suppression of the two-neutrino final state, the standard model contributions to $P\to{\rm invisible}$ decays are dominated by $P\to\barνν\barνν$ processes.

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Rare weak decays of $η^\prime\to Kπ$

Rare weak decays of $η^\prime\to Kπ$ have been investigated in the framework of the $U(3)$ chiral perturbation theory at the leading order. Our study shows that the branching ratio ${\cal B}(η^\prime\to Kπ)$ is of the order of $10^{-11}$, which is far below the present experimental upper bound given by the BESIII Collaboration. By further analysis of $η^\prime\to K^+π^-$ and $η^\prime\to K^0π^0$, the ratio of isospin amplitudes is found that $|A_{1/2}/A_{3/2}|\simeq 35$, which supports that the $ΔI=1/2$ transition enhancement, namely, the $ΔI=1/2$ rule, could be functional in $η^\prime$ weak decays.

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Asymmetries from the interference between Cabibbo-favored and doubly-Cabibbo-suppressed D decays

A phenomenological analysis of $D\to Kπ$ and $D_s^+\to K K $decays including both Cabibbo-favored and doubly-Cabibbo-suppressed modes have been presented by employing the present experimental data. SU(3) symmetry breaking effects from the decay constants and form factors have been taken into account in the analysis. Three asymmetries, $R(D^0)$, $R(D^+)$, and $R(D_s^+)$, which are generated through interference between Cabbibo-favored and doubly- Cabibbo-suppressed decays, are estimated. Theoretical results agree well with the current measurements.

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Analysis of $J/ψ(η_c)\to γ~+$ invisible decays in the standard model

Motivated by the experimental study of $J/ψ\toγ~+$ invisible decay by the CLEO Collaboration, we analyze the process $J/ψ\to γν\barν$, as the standard model background for this invisible decay, at the lowest order. Our investigation shows that Br($J/ψ\to γν\barν$) is far below the present experimental upper limit on the branching ratio of $J/ψ\toγ~+$ invisible, which indicates that some interesting room for new physics in this channel might be expected. We also present a similar analysis of the $η_c\to γν\barν$ decay.

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A note on Higgs decays into $Z$ boson and $J/Ψ(Υ)$

Rare decays $h\to Z V$ with $V$ denoting the narrow $c\bar{c}$ or $b\bar{b}$ resonances, such as $J/Ψ$ or $Υ$ states, have been analyzed. Within the standard model, these channels may proceed through the tree-level transition $h\to ZZ^*$ with the virtual $Z^*\to V$, and also loop-induced process $h\to Zγ^*$, followed by $γ^*\to V$. Our analysis shows that, for the bottomonium final states, the decay rate of $h\to Z Υ$ from the loop-induced process is small and the former transition gives the dominant contribution; while, for the charmonium final states, $Γ(h\to Z J/Ψ)$ and $Γ(h\to ZΨ(2S))$ induced by $h\to Zγ^* \to Z V$ could be comparable to the contribution given by the tree-level $h\to ZZ^*\to Z V$ transition.

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CP mixed property of the Higgs-like particle in the decay channel $h\to Z Z^*\to 4l$

Current experiments do not support, as ATLAS and CMS collaborations at the Large Hadron Collider reported, that the Higgs-like resonance discovered in July 2012 is a pure CP-odd state. We examine a general $hZZ$ vertex which contains CP-even and CP-odd couplings, by studying the process $h\to ZZ^*\to l_1^+l_1^-l_2^+l_2^-$ with $l_1,\, l_2= e$ or $μ$, to explore the CP mixed property of the Higgs-like particle. One momentum asymmetry and two angular asymmetries have been analyzed in order to reveal the difference from different CP-couplings. Our study shows that these asymmetries could be interesting observables in the future precise experiments.

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Higgs decays to $γ$ and invisible particles in the standard model

Using the Higgs boson mass $m_h=125$ GeV, the radiative Higgs decays $h\rightarrowγν_l\barν_l$ with $ν_l = ν_e,\,ν_μ$ and $ν_τ$ are analyzed in the standard model. Our calculation shows that the inclusive width of these processes, i.e., the sum of $Γ(h\toγν_l\barν_l)$ for ${ν_l=ν_e,ν_μ,ν_τ}$, is $1.41$ keV, which is about $15\%$ of $Γ(h\toγγ)$. Therefore, the observation of these channels in the future precise experiments may provide us some useful information on the Higgs physics both in the standard model and in its possible extensions.

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On the angular distributions of tau- --> K_S pi-nu_tau decay

Based on experimental data by the Bell Collaboration, we present a phenomenological analysis of the angular distributions in tau- -->K_S pi-nu_tau decay. Our study shows that the angular analysis could lead to some interesting observables, and the future experimental investigation of these observables might be very helpful in revealing the nature of the scalar components of the decay. New physics contributions from the two-Higgs-doublet model to this decay have also been examined.

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Higgs decays to gamma l+ l- in the standard model

The radiative Higgs decays h -> gamma l+l- with l=e,mu and tau are analyzed in the standard model using m_h=125 GeV. Both tree and one-loop diagrams for the processes are evaluated. In addition to their decay rates and dilepton invariant mass distributions, we focus on the forward-back asymmetries in these modes. Our calculation shows that the forward-backward asymmetries in h -> gamma e+e- and h -> gamma mu+mu- could be up to 10^{-2} while in the tau+tau- final state, these asymmetries are below 1%. Thus the forward-backward asymmetries in h -> gamma l+l- might be interesting observables in the future precise experiments both to test our understanding of Higgs physics in the standard model and to probe the novel Higgs dynamics in new physics scenarios.

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K^+ -> pi^+pi^0e^+e^-: a novel short-distance probe

We study the decay K^+ -> pi^+ pi^0 e^+ e^-, currently under analysis by the NA62 Collaboration at CERN. In particular, we provide a detailed analysis of the Dalitz plot for the long-distance, gamma^*-mediated, contributions (Bremsstrahlung, direct emission and its interference). We also examine a set of asymmetries to isolate genuine short-distance effects. While we show that charge asymmetries are not required to test short distances, they provide the best environment for its detection. This constitutes by itself a strong motivation for NA62 to study K^- decays in the future. We therefore provide a detailed study of different charge asymmetries and the corresponding estimated signals. Whenever possible, we make contact with the related processes K^+ -> pi^+ pi^0 gamma and K_L -> pi^+ pi^- e^+ e^- and discuss the advantages of K^+ -> pi^+ pi^0 e^+ e^- over them.

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A note on the mass splitting of K*(892)

Belle Collaboration reported a new observed value of K*-(892) mass by studying tau --> K_S pi nu_tau decay, which is significantly different from the current world average value given by Particle Data Group 2006. Motivated by this new data, we revisit the issue on the K*0(892)-K*+(892) mass splitting. Our theoretical estimation favors the new measurement by Belle Collaboration. Therefore further experimental efforts are urgently needed to improve our understanding of these issues.

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Strong phases, asymmetries, and SU(3) symmetry breaking in D --> K pi decays

Motivated by some new experimental data, we carry out a phenomenological analysis of D --> K pi decays including both Cabibbo favored and doubly Cabibbo suppressed modes. Two asymmetries, R(D^0) and R(D+), which are generated through interference between Cabbibo favored and doubly Cabibbo suppressed D --> K pi transitions, are predicted. The relative strong phase, delta_{K pi}, between D^0 --> K- pi+ and D^0 --> K+ pi- decays, is estimated. The theoretical results agree well with the current measurements.

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