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Feng Feng

Publications and source records attributed to Feng Feng.

67 records · Page 4Linked to original sources

Lepton number violation in D meson decay

The lepton number violating process can be induced by introducing a fourth generation heavy Majorana neutrino, which is coupled to the charged leptons of Standard Model. There have been many previous studies on the leptonic number violating decay processes with this mechanism, we follow the trend to study the process: $D \to K \ell \ell π$ with the same-sign dilepton final states. We restrict ourself to certain neutrino mass regions, in which the heavy neutrino could be on shell and the dominant contribution to the branching fraction comes from the resonance enhanced effect. Applying the Narrow Width Approximation, we found that upper limit for the branching fractions for $D^0 \to K^-\ell^+\ell^+π^-$ are generally at the order of $10^{-10}$ to $10^{-9}$, if we take the most stringent upper limit bound currently available in the literature for the mixing matrix elements. We also provide the constrains, which is competitive compared to the LNV B decays, on the mixing matrix element $|V_{eN}|^2$ based on the upper limit of $D^0 \to K^- e^+ e^+ π^-$ estimated from Monte-Carlo study at BESIII.

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Automated One-loop Computation in Quarkonium Process within NRQCD Framework

In last decades, it has been realized that the next-to-leading order corrections may become very important, and sometimes requisite, for some processes involving quarkoinum production or decay, e.g., $e^+e^- \to J/ψ+ η_c$ and $J/ψ\to 3γ$. In this article, we review some basic steps to perform automated one-loop computations in quarkonium process within the Non-relativistic Quantum Chromodynamics (NRQCD) factorization framework, and we give an introduction to some related public tools or packages and their usages in each step. We start from generating Feynman diagrams and amplitudes with \textsc{FeynArts} for the quarkonium process, performing Dirac- and Color- algebras simplifications using \textsc{FeynCalc} and \textsc{FeynCalcFormLink}, and then to doing partial fractions on the linear-dependent propagators by \textsc{APart}, and finally to reducing the Tensor Integrals (TI) into Scalar Integrals (SI) or Master Integrals (MI) using Integration-By-Parts (IBP) method with the help of \textsc{Fire}. We will use a simple concrete example to demonstrate the basic usages of the corresponding packages or tools in each step.

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Some recent progress in understanding exclusive double charmonium production at $B$ factories

We review some recent progress in understanding various exclusive double charmonium production processes at $B$ factories, within the nonrelativistic QCD factorization framework. First we investigate the impact of the joint perturbative and relativistic correction on the process that has attracted a great amount of attention in the past decade, $e^+e^-\to J/ψ+η_c$. We then briefly discuss the phenomenological implication of the next-to-leading order perturbative correction to the processes $e^+e^-\to J/ψ+χ_{c0,1,2} (η_{c2})$. We further emphasize a novel theoretical challenge, which is recently discovered by applying the NRQCD factorization approach to the helicity-suppressed hard exclusive reactions involving heavy quarkonium.

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Reconciling the nonrelativistic QCD prediction and the $J/ψ\to 3γ$ data

It has been a long-standing problem that the rare electromagnetic decay process $J/ψ\to 3γ$ is plagued with both large and negative radiative and relativistic corrections. To date it remains futile to make a definite prediction to confront with the branching fraction of $J/ψ\to 3γ$ recently measured by the \textsf{CLEO-c} and \textsf{BESIII} Collaborations. In this work, we investigate the joint perturbative and relativistic correction (i.e. the ${\mathcal O}(α_s v^2)$ correction, where $v$ denotes the characteristic velocity of the charm quark inside the $J/ψ$) for this decay process, which turns out to be very significant. After incorporating the contribution from this new ingredient, with the reasonable choice of the input parameters, we are able to account for the measured decay rates in a satisfactory degree.

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$O(α_s)$ corrections to $J/ψ+χ_{cJ}$ production at $B$ factories

We investigate the ${\cal O}(α_s)$ corrections to $e^+e^-\to J/ψ(ψ')+χ_{cJ}$ ($J=0,1,2$) in the NRQCD factorization approach. These next-to-leading order (NLO) corrections are calculated at the level of helicity amplitude. We have made a detailed analysis for both polarized and unpolarized cross sections, and compared our predictions with the measurements at the $B$ factories. We also derive the asymptotic expressions for each of the NLO helicity amplitudes, and confirm the earlier speculation that at NLO in $α_s$, the double logarithm of type $\ln^2 (s/m_c^2)$ appearing in the NRQCD short-distance coefficient is always associated with the helicity-suppressed channels.

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${\mathcal O}(α_s)$ corrections to $e^+e^-\rightarrow J/ψ+η_{c2}(χ_{c1}^\prime)$ at $B$ factories

We investigate the ${\cal O}(α_s)$ correction to $e^+e^-\to J/ψ+η_{c2}$ in the NRQCD factorization approach. A detailed comparative study between $e^+e^-\to J/ψ+η_{c2}$ and $e^+e^-\to J/ψ+χ^\prime_{c1}$ at $B$ factory energy is also carried out. After incorporating the ${\cal O}(α_s)$ correction, we predict the cross section for the former process to be around 0.3 fb, while that of the latter about 6 times greater. The outgoing $J/ψ$ is found to be dominantly transversely-polarized in the former process, while longitudinally-polarized in the latter. These features may provide valuable guidance for the future experiment to examine the ${}^3P_1$ or ${}^1D_2$ charmonium option of the X(3872) meson through the exclusive double-charmonium production processes. The observation potential of $e^+e^-\to J/ψ+χ^\prime_{c1}$ looks bright for the current data sample of the \textsc{Belle} experiment, provided that the $χ^\prime_{c1}$ is indeed the narrow X(3872) state. In the appendix, we also identify the coefficients of the double logarithms of form $\ln^2(s/m_c^2)$ associated with all the relevant next-to-leading order Feynman diagrams, for the helicity-suppressed double-charmonium production channels $e^+ e^- \to J/ψ+ η_{c2}(η_c,χ_{c0,1,2})$.

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FormLink/FeynCalcFormLink : Embedding FORM in Mathematica and FeynCalc

FORM, a symbolic manipulation system, has been widely used in a lot of calculations for High Energy Physics due to its high performance and fficient design. Mathematica, another computational software program, has also widely been used, but more for reasons of generality and user-friendliness than for speed. Especially calculations involving tensors and noncommutative operations like calculating Dirac traces can be rather slow in Mathematica, compared to FORM. In this article we describe FormLink and FeynCalcFormLink, two Mathematica packages to link Mathematica and FeynCalc with FORM. FormLink can be used without FeynCalc and FeynCalcFormLink, which is an extension loading FormLink and FeynCalc automatically. With these two packages the impressive speed and other special features of FORM get embedded into the generality of Mathematica and FeynCalc in a simple manner. FeynCalcFormLink provides a FORM-based turbo for FeynCalc, making it much more efficient. FormLink turns Mathematica into an editor and code organizer for FORM.

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Exclusive decay of $Υ$ into $J/ψ+χ_{c0,1,2}$

We study the $Υ$ exclusive decay into double charmonium, specifically, the $S$-wave charmonium $ J/ψ$ plus the $P$-wave charmonium $χ_{c0,1,2}$ in the NRQCD factorization framework. Three distinct decay mechanisms, i.e., the strong, electromagnetic and radiative decay channels are included and their interference effects are investigated. The decay processes $Υ(1S,2S,3S)\to J/ψ+χ_{c1,0}$ are predicted to have the branching fractions of order $10^{-6}$, which should be observed in the prospective Super $B$ factory.

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$Apart: A Generalized Mathematica Apart Function

We have generalized the \textsc{Mathematica} function \texttt{Apart} from 1 to $N$ dimension, the generalized function \texttt{\$Apart} can decompose any linear dependent elements in $\mathcal{V}_{x}^*$ to irreducible ones. The elements in $\mathcal{V}_{x}^*$ can be viewed as the corresponding propagators which involve loop momenta, and the decomposition will be useful when one tries to perform the loop calculations using the packages such as \textsc{Fire} and \textsc{Reduze}, which have implemented the integration by parts (IBP) identities and Lorentz invariance (LI) identities. A description on how to use this package, combined with \textsc{Fire}, \textsc{FeynArts} and \textsc{FeynCalc} packages, to do the one-loop calculations in double quarkonium production in $e^+e^-$ colliders is given, and the full source code for a specific process $(e^+e^-\to J/ψ+ η_c)$ is also available.

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$O(α_s v^2)$ correction to $e^+e^-\to J/ψ+η_c$ at $B$ factories

We investigate the ${\mathcal O}(α_s v^2)$ correction to the $e^+e^-\to J/ψ+η_c$ process in the nonrelativistic QCD (NRQCD) factorization approach. Within some reasonable choices of the relative order-$v^2$ NRQCD matrix elements, we find that including this new ingredient of correction only mildly enhances the existing NRQCD predictions. We have also deduced the asymptotic expressions for the ${\mathcal O}(α_s v^2)$ short-distance coefficients, and reconfirm the early speculation that at next-to-leading order in $α_s$, the double logarithm of type $\ln^2 (s/m_c^2)$ appearing in various NRQCD short-distance coefficients is always associated with the helicity-suppressed channels.

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A Recursive Method to Calculate UV-divergent Parts at One-Loop Level in Dimensional Regularization

A method is introduced to calculate the UV-divergent parts at one-loop level in dimensional regularization. The method is based on the recursion, and the basic integrals are just the scaleless integrals after the recursive reduction, which involve no other momentum scales except the loop momentum itself. The method can be easily implemented in any symbolic computer language, and an implementation in Mathematica is ready to use.

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Exclusive decay of P-wave Bottomonium into double J/ψ

We calculate the order-v^2 relativistic correction of J/ψ, including electromagnetic correction, to χ_{bJ}-> J/ψJ/ψ, in the framework of NRQCD factorization formula. The relativistic order-v^2 effect is found to increase the lower-order prediction for the decay width by about 10%, while the electromagnetism contribution is very small about 0.2% for χ_{b0} and χ_{b2}. The total branching ratios are predicted to be of order 10^{-5} for χ_{b0,b2}-> J/ψJ/ψ, but 10^{-11} for χ_{b1}-> J/ψJ/ψ, since there is only electromagnetism contribution in this channel. We predict it is possible to observe these reactions in LHC. Finally, we estimate the decay width and branch ratio of χ_{cJ}-> ωω,ϕϕ) in the constituent quark model by our formula at the leading-order of relativistic correction and electromagnetic correction. The obtained branch ratio of χ_{c0,2}-> ϕϕis in agreement with the experimental measurement in the order of magnitude.

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The criterion for maximally entangled four-qubit state

Paolo Facchi et al.[Phys. Rev. A. 77, 060304(R) (2009)] presented a maximally multipartite entangled state(MMES). Here we give the criterion for four-qubit state.and some new characterizations of the maximally entangled four-qubit state are given.

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