Direct CP violation in Cabibbo-favored charmed meson decays and ϵ′/ϵ in SU(2)L × SU(2)R × U(1)B−L model

Since the standard model contribution is virtually absent, any observation of direct CP violation in the Cabibbo-favored charmed meson decays would be evidence of new physics. In this paper, we conduct a quantitative study on direct CP violation in D0 → K−π+, Ds+ → ηπ+ and Ds+ → η′π+ decays in the SU(2)L ×SU(2)R ×U(1)B−L gauge extension of the standard model. In the model, direct CP violation arises mainly from the interference between the decay amplitude coming from the SM left-left current operators and that from the right-right current operators induced by WR+ gauge boson exchange. Interestingly, the strong phase between the two amplitudes is evaluable, since it stems from difference in QCD corrections to the left-left and right-right current operators, which is a short-distance QCD effect given by ∼αsMWL2/4πlogMWR2/MWL2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ \sim \left({\alpha}_s\left({M}_{W_L}^2\right)/4\pi \right) \log \left({M}_{W_R}^2/{M}_{W_L}^2\right) $$\end{document}. We assess the maximal direct CP violation in the above decays in the SU(2)L × SU(2)R × U(1)B−L model. Additionally, we present a correlation between direct CP violation in these modes and one in K → ππ decay parametrized by ϵ′, since WR+ gauge boson has a sizable impact on the latter.


Introduction
In the standard model (SM), direct CP violation in the Cabibbo-favored charmed meson decays is highly suppressed at the level of O(10 −10 ) [1] because no multiple tree and/or penguin diagrams with different CP phases can interfere. Hence, if discovered, direct CP violation in these modes would immediately be a sign of new physics. This is in contrast to the singly-Cabibbo-suppressed decays, where tree and penguin diagrams in the SM interfere to yield direct CP violation, and also c → ssu and c → ddu processes interfere through long-distance effects and may lead to sizable direct CP violation in the SM [2]. In this paper, we conduct a quantitative study on direct CP violation in Cabibbofavored charmed meson decays with no final-state K 0 , namely, D 0 → K − π + , D + s → ηπ + and D + s → η π + decays, in the SU(2) L × SU(2) R × U(1) B−L gauge extension of the SM. Here, the absence of final-state K 0 ensures that Cabibbo-favored decay amplitudes do not interfere with doubly-Cabibbo-suppressed decay amplitudes via K 0 -K 0 mixing to induce SM contributions to direct CP violation [3,4].
In the SU(2) L × SU(2) R × U(1) B−L model, the right-right current operators, (sc) V +A (ūd) V +A , coming from W + R gauge boson exchange and the left-right current operators, (sc) V ±A (ūd) V ∓A , induced by W + L -W + R mixing both contribute to the Cabibbo-favored decays. However, the Wilson coefficients for the latter are suppressed by ∼ 2m b /m t 1/20 compared to the former if the model naturally accommodates the bottom and top quark Yukawa couplings. Therefore, we assume throughout this paper that the contribution of the right-right current operators dominates over that of the left-right ones. As a support JHEP10(2018)006 for this assumption, we comment that the dominance of the right-right current contribution has been observed in the study [5] of direct CP violation in K → ππ decay in the SU(2) L × SU(2) R × U(1) B−L model, where we have found that the right-right current contribution is larger by factor 5 than the left-right one, which indicates that although the hadronic matrix elements of the left-right operators are enhanced, this is insufficient to overcome the suppression of 2m b /m t 1/20 on their Wilson coefficients.
The hadronic matrix elements of the right-right current operators are simply the minus of those of the left-left current operators, due to parity symmetry of QCD. Nevertheless, the decay amplitude from the right-right current operators and that from the left-left ones acquire a non-trivial relative strong phase from difference in QCD corrections to the rightright and left-left current operators, which manifests itself as a difference between the ratio of the Wilson coefficients for ( Interestingly, this fact allows us to evaluate the relative strong phase, since the difference in QCD corrections at scales between µ ∼ M W R and µ ∼ M W L is a short-distance effect. Also, the scale-and-scheme-independent combinations [6] of Wilson coefficients and hadronic matrix elements for ( operators can be estimated reliably with the diagrammatic approach with SU(3) flavor symmetry [7][8][9][10][11], which works successfully on the Cabibbo-favored charmed meson decays into two pseudoscalars [12,18]. 1 Combining the strong phase thus evaluated and new CP-violating phases in the SU(2) L × SU(2) R × U(1) B−L model, we assess the maximal direct CP violation in D 0 → K − π + , D + s → ηπ + and D + s → η π + decays. Additionally, we investigate a correlation between direct CP violation in the above modes and one in K → ππ decay parametrized by . Previously, the authors have found [5] that W + R gauge boson in the SU(2) L × SU(2) R × U(1) B−L model with 'charge symmetry' [19] has a sizable impact on / because W + R exchange contributes to it at tree level. It has been further revealed that the model with O(10) TeV W + R boson mass can account for the incompatibility between the experimental data on / [20 -22] and the upper bound on / [23,24] obtained with dual QCD approach and supported by lattice-based evaluations [25][26][27][28][29][30]. 2 Therefore, it is of particular interest how / and direct CP violation in Cabibbo-favored charmed meson decays are correlated in the SU(2) L × SU(2) R × U(1) B−L model, and how the former constrains or predicts the latter. This paper is organized as follows: In section 2, we briefly review the SU(2) L ×SU(2) R × U(1) B−L gauge extension of the SM. In section 3, we give the effective Hamiltonian for the Cabibbo-favored charmed meson decays. Section 4 presents our new results, where the diagrammatic amplitudes are reorganized in such a way that the decay amplitude coming from 1 Earlier studies on the application of the diagrammatic approach with SU(3) flavor symmetry to charmed meson decays into two pseudoscalars are found in refs. [13,14] and in refs. [15][16][17].

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We briefly describe the SU(2) L ×SU(2) R ×U(1) B−L gauge extension of the SM. Remind that charge symmetry [19] is not imposed, unlike ref. [5]. We summarize the matter content in table 1. SU(2) L × SU(2) R × U(1) B−L gauge interactions and Yukawa interactions of quarks are described as ∆ R acquires a VEV, v R , to break SU(2) R ×U(1) B−L → U(1) Y , and Φ further gains a VEV, Φ = diag(v sin β, v cos βe i α ) with v 246 GeV, to trigger the electroweak symmetry breaking. As a result, the charged SU(2) L gauge boson, W + L , and the charged SU(2) R gauge boson, W + R , mix and form two mass eigenstates W + , W + as The up-type quark mass matrix, M u , and the down-type one, M d , are given by 3 Then, we obtain the SM Cabibbo-Kobayashi-Maskawa matrix as V L = V uL V † dL , and the corresponding flavor mixing matrix for right-handed quarks as V R = V uR V † dR . From eq. (2.2), we find that the charged-current interactions are described by the following term in the unitary gauge: From eq. (2.4), it is clear that the top and bottom Yukawa couplings are derived without fine-tuning only when tan β m b /m t holds, which, combined with eq. (2.3), gives . Then, one finds from eq. (2.5) that the Wilson coefficients for the left-right currents obtained by integrating out W + are suppressed by 2m b /m t compared to those for the right-right currents obtained by integrating out W + .

Effective Hamiltonian for Cabibbo-favored ∆C = 1 process
The effective Hamiltonian for Cabibbo-favored ∆C = 1 process reads, The operators above are defined as where (qq ) V −A and (qq ) V +A stand forqγ µ (1−γ 5 )q andqγ µ (1+γ 5 )q , respectively, and α, β denote QCD color indices. C LL i (i = 1, 2) in eq. (3.1) represents the SM contribution, while C RR i arises from W + R gauge boson exchange. In this paper, we neglect the left-right current The renormalization group equation (RGE) of the Wilson coefficients is divided into two pieces for chirality-flipped sectors. At leading order, it reads T , and the anomalous dimension matrix γ is common for LL and RR sectors. The initial conditions for the RGE at leading order are so that the RG evolution is simply described without operator mixing.

Decay amplitudes from right-right current operators
Hereafter, we exclusively work under the assumption of SU(3) flavor symmetry of u, d, s quarks. The amplitudes of charmed meson decays to two pseudoscalars (D → P P ) can be categorized by diagrammatic topologies [12][13][14][15][16][17][18]. For the Cabibbo-favored D → P P decays, the diagrammatic amplitudes consist of T (tree), C(color-suppressed tree), A(annihilation) and E(exchange) diagrams. In addition, ref. [6] has clarified the correspondence between the diagrammatic amplitudes and the scale-and-scheme-independent combinations of Wilson coefficients and operators.
For the left-left and right-right current contributions, the diagrammatic amplitudes are rewritten as where µ denotes a common renormalization scale for the Wilson coefficients and operators of both left-left and right-right currents. Q i (µ) denotes a hadronic matrix element defined by Q i (µ) = P P | Q LL i (µ) |D , whose subscript represents the connected emission (CE), the disconnected emission (DE), the connected annihilation (CA) and the disconnected annihilation (DA), respectively [6]. We have used P P | Q LL i (µ) |D = − P P | Q RR i (µ) |D (i = 1, 2) that follows from parity conservation of QCD. We emphasize that each of T LL , T RR , C LL , C RR , A LL , A RR , E LL , E RR is independent of renormalization scale and scheme [6].
The diagrammatic amplitudes have been determined through a phenomenological fitting of D → P P decay partial widths in ref. [12] (see also ref. [18]). In that study, an important assumption is that OZI-suppressed diagrams for D 0 →K 0 η, D 0 →K 0 η , D + s → π + η, D + s → π + η decays are negligible in the partial widths. Also, the SU(3) flavor symmetry is assumed. These assumptions are justified for the Cabibbo-favored decays, since a good fit with χ 2 = 1.79 for 1 degree of freedom for fixed η − η mixing angle is obtained in JHEP10(2018)006 that study. 4 In this paper, we employ the result of ref. [12] by fixing the η − η mixing angle at 19.5 • . Assuming that the contributions of the right-right current operators to the partial widths are negligible, one finds [12]

Numerical analysis on direct CP violation
In the SM, direct CP violation in the Cabibbo-favored decays is generated via the interference between the tree diagram and the box and di-penguin diagrams [1]. CP asymmetry in D 0 → K − π + decay rate is estimated to be 1.4 × 10 −10 in ref. [1]. We infer that direct CP violation is suppressed similarly in all Cabibbo-favored modes, and therefore neglect the SM contribution in all modes. Provided the contribution of the right-right current is small, CP asymmetry in the decay rates can be expanded as The diagrammatic amplitude of each Cabibbo-favored decay is given in table 2. By using the relations eqs. (4.13)-(4.16) and the leading order expression for the Wilson coefficient ratio eq. (4.17), we find that the asymmetry takes a simple form, where F D→f CP is a process-dependent factor, which is summarized in table 2. The QCD correction factor and CP phase dependence in eq. (5.2) are common for all Cabibbofavored modes. Note that A D 0 →K 0 π + CP vanishes because T RR + C RR and T LL + C LL have an identical strong phase. In appendix A, NLO QCD corrections with the appropriate threshold corrections at the matching scales µ W and µ W , which we use in the numerical analysis, are given.
In figure 1, maximal CP asymmetries in D 0 → K − π + , D + s → π + η and D + s → π + η in the SU(2) L × SU(2) R × U(1) B−L are plotted by taking Im V R * cs V R ud /V L * cs V L ud = 1/ cos 2 θ C (θ C denotes the SM Cabibbo angle). To estimate theoretical uncertainty, we have varied the matching scales µ W and µ W in the range M W /2 ≤ µ W ≤ 2M W and M W /2 ≤ µ W ≤ 2M W , respectively. Also, the 1σ errors of the diagrammatic amplitudes in ref. [12] are considered as a source of uncertainty. We observe in figure 1 that the asymmetry is specially enhanced in D + s → π + η decay, due to the relatively large process-dependent factor. Note that we do not study the other Cabibbo-favored decays, because they include a final-statē K 0 and are thus observed via K 0 -K 0 mixing. Hence, the amplitudes of Cabibbo-favored and doubly-Cabibbo-suppressed decays interfere to yield non-negligible CP asymmetry in the SM.

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In real experiments, one measures the difference of the CP asymmetries in two processes, to nullify asymmetry in the production cross sections at pp colliders or a slight asymmetry in the production kinematics at e + e − colliders (due to Z-photon interference), and asymmetry in the efficiency of charged meson detection. Consequently, most of the systematic uncertainties cancel. For the search for direct CP violation in Cabibbo-favored decays in the SU(2) L × SU(2) R × U(1) B−L model, we suggest that one measure because the two asymmetries are predicted to have opposite signs in table 2 (note the signs of F D→f CP ) and A D + s →π + η CP is sizable. Also, asymmetries in the D ± s production and the π ± detection efficiency largely cancel between the two processes. In figure 2, we plot the maximal difference in the CP asymmetries in D + s → π + η and D + s → π + η by again taking Im V R * cs V R ud /V L * cs V L ud = 1/ cos 2 θ C . We comment that, as shown in appendix B, our prediction for the CP asymmetry difference eq. (5.3), which has been derived by assuming SU(3) flavor symmetry, is not much affected by SU(3) flavor symmetry breaking.
We make a crude estimate on the statistical uncertainty in a measurement of eq. (5.3) at Belle II with 50 ab −1 of data. Reference [44] reports that with 791 fb −1 of data at Belle, statistical uncertainty of the CP asymmetry in the number of reconstructed events (N rec (D → f ) − N rec (D →f ))/(N rec (D → f ) + N rec (D →f )) is 1.13% for D + → π + η and 1.12% for D + → π + η . Assuming that the signal efficiencies (1.6%-1.7%) are the same for D + → π + η( ) and D + s → π + η( ), and using the branching ratios found in ref. [45], we estimate the statistical uncertainty at Belle II with 50 ab −1 of data to be ∆(A D + .08%. Next, we estimate the statistical uncertainty in a measurement of eq. (5.3) at LHCb with 50 fb −1 of data. Reference [46] reports that with 1 fb −1 of data at 7 TeV and 2 fb −1 of data at 8 TeV LHCb, the signal yield of D ± s → π ± η processes is 152×10 3 . Making a rough approximation that the signal yield with 2 fb −1 of data at 8 TeV is twice the yield with 1 fb −1 of data at 7 TeV, and performing a naïve rescaling of the number of events by ×200 based on ref. [47], the signal yield of D ± s → π ± η processes with 50 fb −1 of data is estimated to be 10 7 . Further assuming that the signal efficiencies for D ± s → π ± η and D ± s → π ± η are the same, the statistical uncertainty with 50 fb −1 of data is found to be ∆(A D + s →π + η CP − A D + s →π + η CP ) =0.06%. We find that if the SU(2) R gauge coupling is enhanced as g R = 2g L , one may hope to discover direct CP violation in Cabibbo-favored decays even with M W = 4 TeV (this parameter point is nearly consistent with the bound on Z derived in refs. [49,50]).
In figure 3, a correlated prediction for the CP asymmetry difference A D + and Re( / ) calculated in ref. [5] in the SU(2) L × SU(2) R × U(1) B−L model is presented. Here, as with ref. [5], we impose 'charge symmetry' [19] on the model, which gives g L = g R and V R ud = (V L ud ) * e −i ψ d , V R cs = (V L cs ) * e i(φc−ψs) , V R us = (V L us ) * e −i ψs with ψ d , ψ s , φ c being arbitrary CP-violating phases. We thereby forbid ad hoc tuning of model parameters, rendering the model more predictive. In our calculation of Re( / ), we have considered all contributions including those from the left-right current operators, unlike in our calculation of direct CP violation in D → P P decays. In the plot, ψ d , ψ s , φ c and α JHEP10(2018)006 Table 2. Diagrammatic amplitudes [12], process-dependent factors for CP asymmetry, and their numerical values for Cabibbo-favored charmed meson decays. The uncertainty comes from the 1σ errors of the diagrammatic amplitudes. Here, we fix the η − η mixing angle at arcsin(1/3).
(which appears in eq. (2.2)) are randomly generated in the range [0, 2π]. We observe that when the experimental value of Re( / ) is naturally accounted for, the CP asymmetry difference is about 10 −6 . Conversely, to have A D + s →π + η CP − A D + s →π + η CP as large as 10 −4 , one must fine-tune the new CP-violating phases to satisfy the 1σ range of Re( / ).
We comment in passing that for W + R gauge boson in the SU(2) L × SU(2) R × U(1) B−L model, the constraint from indirect CP violation in kaons, Re( ), is mild compared to that from direct CP violation Re( / ), because W + R gauge boson exchange contributes to the latter at tree level while it contributes to the former only at loop levels. However, it should be noted that unless the scalar potential is fine-tuned, the contribution from the heavy neutral scalar exchange to Re( ) is sizable, which is investigated in detail in refs. [51,52].

Summary
We have studied the contribution of the right-right current operators in the SU(2) L × SU(2) R ×U(1) B−L model to direct CP violation in Cabibbo-favored charmed meson decays, for which the SM contribution is virtually absent. Interestingly, this contribution is evaluable, because it stems from difference in QCD corrections to the left-left current operators induced by W + L boson and the right-right ones induced by W + R boson, which is a short- . Combining a short-distance calculation of this difference with the result of the diagrammatic approach to the Cabibbo-favored decay amplitudes, we numerically evaluate the CP asymmetry in D 0 → K − π + , D + s → π + η JHEP10(2018)006  and D + s → π + η decay rates. We have found that the asymmetry in D + s → π + η is specially sizable, and further suggested the measurement of the difference in the CP asymmetries in D + s → π + η and D + s → π + η decays. For M W (almost equal to M W R ) about 4 TeV and g R = 2g L , one may hope to observe this CP asymmetry difference at Belle II with 50 ab −1 of data or at LHCb with 50 fb −1 of data. Finally, we have presented a correlated prediction for the CP asymmetry difference in D + s → π + η and D + s → π + η decays, and direct CP violation in K → ππ decay Re( / ), under the assumption of 'charge symmetry' in the SU(2) L × SU(2) R × U(1) B−L model. We have observed that if the experimental data on Re( / ) are naturally accounted for, the CP asymmetry difference in D + s → π + η and D + s → π + η decays is as small as 10 −6 , and that a fine-tuning of the new CP-violating phases is mandatory to anticipate the discovery of direct CP violation in Cabibbo-favored charmed meson decays.

A NLO formulas
Here, we summarize NLO QCD corrections to the observables which are discussed in this paper. At NLO, the ratio of the Wilson coefficients in eq. (4.17) is modified to where β 1 is the six-flavor NLO QCD β function coefficient, λ 1± are the NLO γ function coefficients for C LL ± and C RR ± , and B ± are constants (see, e.g., ref. [53]). Note that each of λ 1± and B ± is renormalization-scheme-dependent, but their scheme dependences cancel. Thus at NLO, the CP asymmetry in eq. (5.2) is

B Effect of SU(3) flavor symmetry breaking
We study the effect of SU(3) flavor symmetry breaking on our prediction, which is not discussed in the main text. Our prediction of CP asymmetries depends crucially on Vspin symmetry (symmetry of u and s, which is part of SU(3) flavor symmetry), since our prediction is derived from eqs. (4.5)-(4.8), which are obtained by assuming V-spin. In particular, the isospin symmetry cannot lead to the above results. The effect of V-spin breaking on eqs. (4.5)-(4.8) is estimated to be simply f K /f π − 1 0.2. This is in contrast to singly-Cabibbo-suppressed decays, where SU(3) breaking gives rise to corrections of order (f K /f π ) 2 − 1 0.4 in factorized tree amplitudes, and also enhances penguin amplitudes (suppressed by V cb V * ub in the SU(3) limit) leading to a further splitting of c → dduinduced amplitudes and c → ssu-induced amplitudes [54]; all these effects are absent in the Cabibbo-favored decays.
Let us see how corrections of order f K /f π − 1 0.2 to eqs. (4.5)-(4.8) affect our prediction of CP asymmetries. First we concentrate on T (tree) and C(color-suppressed tree) diagrams. When eqs. (4.5), (4.6) are not valid, T LL and C LL are written as 2) The first and second terms on the right-hand side of eqs. (B.1), (B.2) are individually renormalization-scale-and-scheme independent. Therefore, we can parametrize the V-spin breaking effects in terms of renormalization-scale-and-scheme independent parameters E+ and E− as where we estimate the V-spin breaking parameters as In the leading order of E+ , E− , we find Consequently, T RR and C RR can be expressed in terms of T LL , C LL and the V-spin breaking parameters as We obtain analogous expressions for A RR and E RR , with E+ , E− replaced with different V-spin breaking parameters A+ , A− . The above V-spin breaking corrections solely affect the factor F D→f CP in the formula for CP asymmetry eq. (5.2). For the phenomenologically interesting modes D + s → π + η, D + s → π + η and D 0 → K − π + , this factor is altered from table 2 to

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Depending on the phases of V-spin breaking parameters E+ , E− , A+ , A− , the second and third terms of eqs. (B.9)-(B.11) can be enhanced far beyond f K /f π − 1 0.2. However, as we will show below, the most promising observable, A D + s →π + η CP − A D + s →π + η CP , is not much affected by the V-spin breaking. To see this, note that this observable is proportional to F D + s →π + η CP − F D + s →π + η CP . Since |A LL | is small, it can be approximated as where the first term −1.54 is the prediction in the V-spin limit, while the second and third terms represent V-spin breaking effects. The second term is at most ±3|E LL /T LL |(f K /f π − 1) ±0.32 and the third term is at most ±3|A LL /T LL |(f K /f π − 1) ±0.07. Thus, we conclude that the V-spin breaking corrections do not significantly change our prediction of We note in passing that the fitted values of T LL , C LL , E LL , A LL in ref. [12], which we have adopted throughout the paper, are themselves obtained under the assumption of SU(3) flavor symmetry, but we expect that the SU(3) breaking effects are properly reflected in the errors of the fitted values.
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