K 0 S (cid:0) K 0 L asymmetries and CP violation in charmed baryon decays into neutral kaons

: We study the K 0 S (cid:0) K 0 L asymmetries and CP violations in charm-baryon decays with neutral kaons in the (cid:12)nal state. The K 0 S (cid:0) K 0 L asymmetry can be used to search for two-body doubly Cabibbo-suppressed amplitudes of charm-baryon decays, with the one in (cid:3) + c ! pK 0 S;L as a promising observable. Besides, it is studied for a new CP -violation e(cid:11)ect in these processes, induced by the interference between the Cabibbo-favored and doubly Cabibbo-suppressed amplitudes with the neutral kaon mixing. Once the new CP-violation e(cid:11)ect is determined by experiments, the direct CP asymmetry in neutral kaon modes can then be extracted and used to search for new physics. The numerical results based on SU(3) symmetry will be tested by the experiments in the future.


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violation compared to the SM prediction [31][32][33][34]. Therefore, it is important to search for the two-body DCS amplitudes of charm-baryon decays. Except for the direct measurement on the DCS processes, the two-body DCS amplitudes can also be revealed by the K 0 S − K 0 L asymmetry in charmed baryon decays into neutral kaons. The K 0 S − K 0 L asymmetry is induced by the interference between the CF and DCS amplitudes, which has been studied in D meson decays [33,[35][36][37][38][39][40][41]. In this work, we investigate the K 0 S − K 0 L asymmetry in charmed baryon decays, and find that the one in Λ + c → pK 0 S,L is the promising observable to search for two-body DCS charm-baryon decay amplitudes.
CP violation can occur in charmed baryon decays into neutral kaons. It is an essential element to interpret the matter-antimatter asymmetry in the Universe [42] and provides a window to search for new physics beyond the SM. CP asymmetries have been well established in kaon and B meson systems [30]. In the baryon sector, the only signal of CP asymmetry is found in Λ 0 b → pπ − π + π + with 3.3 σ [43]. CP violation in charmed baryon decays has not been observed up to now. In some literatures, the CP violation in charm decays into neutral kaons have be studied [31,34,[44][45][46][47][48]. In ref. [49], a new measurable CP -violation effect is found existing in D meson decays into neutral kaons, except for the known indirect CP violation in K 0 − K 0 mixing and direct CP asymmetry in charm decays. The new effect is induced by the interference between the CF and DCS amplitudes with the mixing of final-state mesons. In this work, we will show that the new CP -violation effect also exist in charmed baryon decays. Once the new effect was well determined in experiment, the direct CP asymmetry could be obtained and used to search for new physics.
This paper is organized as follows. In section 2, we discuss the K 0 S − K 0 L asymmetry in charmed baryon decays into neutral kaons and its search for the DCS transitions. The corresponding time-dependent and time-integrated CP asymmetries are studied in section 3. The numerical analysis is given in section 4. And section 5 is the summary.
In the charmed hadron decays into neutral kaons, the interference between the Cabibbofavored (CF) and the doubly Cabibbo-suppressed (DCS) amplitudes leads to the K 0 S − K 0 L asymmetry, an observable to search for the DCS transitions. Specifically, the K 0 S − K 0 L asymmetry in charmed baryon (B c ) decaying into light baryon (B) and neutral kaons is defined as .

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Due to the fact that the K 0 S − K 0 L asymmetry is not sensitive to the CP violating effect in the K 0 − K 0 mixing [40], the K 0 S and K 0 L states can be referred as the CP eigenstates The CF amplitude of B c → BK 0 and the DCS amplitude of B c → BK 0 decays read as where T CF (T DCS ) is the magnitude of the CF (DCS) amplitude, and δ CF (δ DCS ) and φ CF (φ DCS ) are the relative strong and weak phases, respectively. The decay amplitudes of B c → BK 0 S and B c → BK 0 L are then Similar as ref. [40], the ratio between the DCS and CF amplitudes are defined as The parameters r f and δ f depend on the individual processes, while φ is mode independent in the SM. It is found that if the DCS amplitude vanishes, r f = 0. In the SM, r f is expected to be proportional to the ratio |V * cd V us /V * cs V ud | ∼ λ 2 ∼ O(10 −2 ), and the weak phase is negligibly small, i.e., φ ≡ Arg[−V * cd V us /V * cs V ud ] = (−6.2 ± 0.4) × 10 −4 . The K 0 S − K 0 L asymmetry can be further reduced as [40] R(B c → BK 0 S,L ) = which is expected to be of the order of O(10 −2 ), being measurable in experiments. The K 0 S − K 0 L asymmetry could be used to search for the DCS decays in charmed baryon decays. If the DCS transition is absent, i.e., r f = 0, the K 0 S − K 0 L asymmetry shall vanish. Thereby, a non-zero experimental result of R(B c → BK 0 S,L ), namely r f = 0, can be taken as the evidence for the DCS transitions of charmed baryons. In fact, since the branching fraction of Λ + c → pK 0 S is measured as [9] Br(Λ + c → pK 0 S ) exp = (1.52 ± 0.08 ± 0.03)%, (2.7) it can be expected that Λ + c → pK 0 L has a branching fraction of the order of one percent, and thus might be measured with large data sample. Therefore, the corresponding K 0 S − K 0 L asymmetry can reveal the DCS amplitude of Λ + c → pK 0 .

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In the following discussions, we will see that the K 0 S − K 0 L asymmetry in the decays of Λ + c → pK 0 S,L is a promising observable to search for the two-body DCS amplitude of charmed baryon decays. At BESIII, only Λ + c can be produced due to the energy limit. At Belle (II) and LHCb, the productions of Ξ + c and Ξ 0 c with an additional strange quark are smaller than Λ + c . For the two-body Λ + c decays into the light baryon octet and a pseudoscalar meson, the only two DCS modes are Λ + c → pK 0 and Λ + c → nK + . In the latter mode, neutron is always difficult to be detected in experiments. On the contrary, Λ + c → pK 0 can be revealed by the K 0 S − K 0 L asymmetry in Λ + c → pK 0 S,L with K 0 L detected with a high efficiency at Belle (II). In the decay modes of Λ + c into the baryon octet and a vector meson, and the baryon decuplet and a pseudoscalar meson, the DCS transitions include Λ + c → pK * 0 , nK * + , ∆ + K 0 , ∆ 0 K + . Among them, the decays of Λ + c → nK * + (→ K + π 0 ) and Λ + c → K 0 ∆ + (→ pπ 0 ) suffer from the low efficiencies of detections of neutrons or π 0 . The modes of Λ + c → pK * 0 (→ K + π − ) and Λ + c → K + ∆ 0 (→ pπ − ) are actually included in the measured three-body DCS decay Λ + c → pK + π − [10], while a partial-wave analysis requires much more data. In short, the K 0 S − K 0 L asymmetry in Λ + c → pK 0 S,L decays is of a priority to investigate the two-body DCS charm-baryon-decay amplitudes in experiments, especially at Belle (II).

CP asymmetry
CP violation can occur in the charm decays into neutral kaons, induced by the interference between the CF and DCS amplitudes with the K 0 −K 0 mixing. As pointed out in [49], there exist three CP -violation effects in charmed meson decays, i.e., the indirect CP violation in K 0 − K 0 mixing, the direct CP asymmetry in charm decays, and the effect from the interference between two tree (CF and DCS) amplitudes with neutral kaon mixing. It is also worthwhile to study the CP -violation effects in the charmed baryon decays. Unlike eq. (2.2), the indirect CP violation in K 0 − K 0 mixing should be taken into account for the study of CP violation effects in charmed baryon decays. Such that the K 0 S and K 0 L states are , and is a small complex parameter characterizing the indirect CP asymmetry in the K 0 − K 0 mixing system, with the values of | | = (2.228 ± 0.011) × 10 −3 and its phase φ = 43.52 • ± 0.05 • [30]. In experiments, the K 0 S state is actually reconstructed by π + π − . The time-dependent CP asymmetry in the decay chain of B c → BK(t)(→ π + π − ) reads as and t is the time difference between the charmed baryon decays and the neutral kaon JHEP03(2018)066 decays in the kaon rest frame [47,49]. The amplitude of A(B c → BK(t)(→ π + π − )) can be deduced as in which g + and g − describe the flavor preserving and flavor changing time evolutions, respectively, with the mass m S (m L ) and the width Γ S (Γ L ) of the K 0 in the numerator denotes the CP violation in neural kaon mixing [47], , independent on the DCS amplitude. The second term A dir CP (t) is the direct CP asymmetry induced by the interference between the CF and DCS amplitudes, The third term A int CP (t) originates from the interference between the two tree (CF and DCS) amplitudes with the neutral kaon mixing, A int CP (t) has been missed in the literature of studying D meson decays [31,34,[46][47][48] in which the DCS amplitudes are assumed to be zero, and was first pointed out in [49] as a new CP -violation effect. It arises from the mother decay and the daughter mixing. Its physical meaning can be depicted in figure 1, a schematic description of the chain decay, taking Λ + c → pK(t)(→ π + π − ) as an example. A int CP (t) is from the interference effect between the Cabibbo-favored amplitude of Λ + c → pK 0 with neutral kaon mixing K 0 → K 0 (t) → π + π − , and the doubly Cabibbo-suppressed amplitude of Λ + c → pK 0 without kaon mixing K 0 → K 0 (t) → π + π − . Equivalently, the new CP -violation effect is also from the interference effect between the amplitudes of Λ + c → pK 0 without kaon mixing is from the (daughter) kaon mixing, , while the strong phase is from JHEP03(2018)066 Figure 1. Schematic description of the chain decay Λ + c → pK(t)(→ π + π − ). the (mother) charm decays, δ f . Its mechanism is more complicated than for the ordinary mixing-induced CP asymmetry in, for instance, the D 0 (t) → K + K − mode, in which both the oscillation and decay take place in the mother particle D 0 (t). Besides, A int CP (t) isn't the direct CP asymmetry in charm decays, since it doesn't vanish as φ → 0. In order to investigate the direct CP violation A dir CP (t) which is tiny in the SM due to the smallness of φ and thus sensitive to new physics, it is necessary to extract A K 0 CP (t) and A int CP (t) from the total CP violation, seen in eq. (3.5). Thus it is worthwhile to study A int CP (t) in the relevant processes. In eq. (3.8), neglecting the weak phase in charm, i.e., setting φ → 0, only r f and δ f are required to predict the values of A int CP (t), since is well determined in experiment. Fortunately, r f and δ f can be obtained by the data of branching fractions, which will be discussed in section 4.
From eqs. (3.6) ∼ (3.8), it is found that A K 0 CP (t) and A int CP (t) vanish at t = 0 and In the SM, A CP (t = 0) is of order of 10 −5 since r f ∼ O(10 −2 ) and φ ∼ O(10 −4 ). Such an order is far beyond the precision limit of the forthcoming experiments, Belle II and LHCb upgrade. However, in some new physics models, the weak phase difference can be large, which results in a larger A CP (t = 0). Thereby, an observation with nonvanishing A CP (t = 0) would be the signal of new physics [49]. Unlike the SCS processes, in which the precise measurement of the CP asymmetry cannot discriminate new physics due to the ambiguities in estimating the penguin amplitudes, the measurable direct CP asymmetry in B c → BK(t)(→ π + π − ) indicates new physics effect because of its tiny value in the SM. The time-integrated CP asymmetry is covered by the bare asymmetry with a timedependent function, F (t), introduced to take into account relevant experimental effects, . (3.10)

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In this work, we adopt the approximation in [47] F (t) = 1 t 1 < t < t 2 , 0 t > t 2 or t < t 1 . (3.11) Eq. (3.10) is reduced as in which x ≡ ∆m/Γ, c(t) = e −Γt [cos(∆mt) − x sin(∆mt)], and s(t) = e −Γt [x cos(∆mt) + sin(∆mt)]. The first term, being independent of t 1,2 , corresponds to the direct CP asymmetry in charm decays. In the rest part of eq. (3.12), the terms proportional to r f represent the new effect A int CP (t 1 , t 2 ), and those without r f are the CP violation in the neutral kaon mixing.
In the limitation of t 1 τ S t 2 τ L , e −Γt 1 = e −Γ S t 1 = 1 and e −Γt 2 = e −Γ S t 2 = 0. The time-integrated CP violation then reads as Considering the sizes of , r f and φ, the interference between charm decays and neutral kaon mixing A int CP is expected to be of the order of O(10 −4∼−3 ). Such an order is much larger than the direct CP violation in charm decays.
In eq. (3.14), the 2r f cos φ cos δ f term in the denominator cannot be neglected, since the new CP -violation effect, 4r f Im[ ] cos φ sin δ f , is a sub-leading contribution which is at the same order as the term in the denominator by expansion to be 4r f Re[ ] cos φ cos δ f . The 2r f cos φ cos δ f term can be determined by the measurement of the K 0 S −K 0 L asymmetry since the weak phase φ is tiny in the SM, In the case of D + → π + K 0 S decay, the term in the denominator is one order of magnitude smaller than the new CP -violation effect and can be neglected [49], since R(D + → π + K 0 S ) is measured to be small [41] R(D + → π + K 0 S,L ) = 0.022 ± 0.016 ± 0.018. (3.16)

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But in the case of Λ + c → pK 0 S , the contribution from the denominator can only be determined by the measurement of the K 0 S − K 0 L asymmetry. The time-dependent and time-integrated CP violation in Λ + c → pK 0 S can be measured by Belle II and LHCb. In order to extract the new CP -violation effect A int CP , we propose an observable, where D in the last line is the denominator of eq. (3.14). The CP violation in neutral kaon mixing is mode-independent and thus cancelled between the ones in Λ + c → pK 0 S and D + → π + K 0 S . As discussed above, the direct CP violation is negligible. Therefore, the new CP -violation effect can be revealed in ∆A CP (K 0 S , p, π + ). It can be measured at LHCb by combination of the raw asymmetries A raw with those in CF channels, canceling the production and detection asymmetries, as

Numerical analysis
In the this section, we numerically estimate the K 0 S −K 0 L asymmetries and CP asymmetries in charmed baryon decays into neutral kaons based on the flavor SU(3) symmetry. The CF and DCS processes are model-independently analyzed with the parameters extracted from experimental data. In this work, we focus on the decays of the charmed-baryon anti-triplet (Ξ 0 c , −Ξ + c , Λ + c ) into light baryon octet and pseudoscalar octet. Note that sizable flavor SU(3) breaking effect is always expected in charmed hadron decays. It is found to be very large in the SCS processes of D decays, like the difference between D 0 → K + K − and π + π − . However, the SU(3) symmetry seems to work well in the CF processes. For example, in the analysis of D meson decays using the topological diagrammatic approach under the SU(3) symmetry in ref. [39], the fitted results show that χ 2 /d.o.f = 0.65 for a global fit with only CF processes, while χ 2 /d.o.f = 87 in the case with only SCS processes. Since we focus on the charmed baryon decays into neutral kaons in the CF and DCS processes in this work, the SCS processes are not involved in the global fit. Thus large SU(3) breaking effects can be avoided. Besides, unlike the D 0 decays into neutral kaons in which the strong phase difference δ f = 0 in the flavor SU(3) limit [40,[50][51][52][53][54] and thus A int CP ∝ sin δ f is unobservable, δ f and A int CP are non-vanishing in the charged D-meson decays [49,55,56]. In charmed baryon decays, it will be found in the following that the CF and DCS amplitudes are different in the SU(3) decomposition, inducing non-vanishing δ f and A int CP . The nonleptonic charmed decays are induced by the operators (sc)(ūd) for the CF modes, and (dc)(ūs) for the DCS modes. These operators can be decomposed into irreducible representations of flavor SU (3) [57,58]. In an approximation of neglecting the contributions from O 15 , the effective Hamiltonian is expressed as [20,21,27] with the charmed-baryon anti-triplet the light baryon octet, and the pseudoscalar octet The non-zero elements H 22 (6) = 2 for Cabibbo-allowed modes, and H 33 (6) = 2 tan 2 θ C for doubly Cabibbo-suppressed modes, where θ C is the Cabibbo angle and tan 2 θ C |V * cd V us /V * cs V ud |. The coefficients e, f, g are free complex parameters to be extracted from data of branching fractions.
The partial decay width of charmed baryon decays is where p c is the center-of-mass momentum of the final state particles, m Bc and m B are the masses of charmed baryon and light baryons. The decay amplitudes are expressed by the e, f , g parameters, with the representations given in table 1. Since only the relative phases between e, f and g make sense, we take e as real. At the current stage, the available relevant data include five branching fractions of CF decays of Λ + c (shown in table 1) and the ratio of branching fractions between Ξ 0 c → ΛK 0 S and Ξ 0 c → Ξ − π + . So then five free parameters are fixed by six data via a global fit. Notice that f and g always occur together as (f + g) in the CF amplitudes, we use h = f + g in the fit to avoid large correlation, and g can be obtained through g = h − f . Then we find e = 0.67 ± 0.03, |f | = 0.26 ± 0.03, h = f + g = (0.43 ± 0.06) e i(0.97±0.06) , (4.6) with χ 2 /d.o.f = 0.17, and the phase of f ranges from −π to π. One can find the magnitudes of |e| and |f | are mostly fixed by Λ + c → pK 0 S and Ξ 0 K + , respectively, where the DCS contribution in the pK 0 S mode is highly suppressed. The parameter h is also well determined JHEP03(2018)066  Table 1. Branching fractions and amplitude representations for the Cabibbo-favored charmed baryon decays. For the modes with neutral kaons K 0 S,L in the final states, the associated doubly Cabibbo-suppressed amplitudes are taken into account with the factor of tan 2 θ C . The ratio of BR(Ξ 0 c → ΛK 0 S )/BR(Ξ 0 c → Ξ − π + ) = 0.210 ± 0.028 is also included in the global fit. Our results are given in the last column, compared to the experimental data [30]. by global fitting. The phase of f cannot be extracted from the available data, and thus is free in the full range between −π and π. The numerical results of branching fractions are given in the last column in table 1, compared to the experimental data [30]. The uncertainties in our predictions include the errors from the global fit and the ones from the lifetimes of Λ + c , Ξ + c and Ξ 0 c . For those modes in which g occurs without f , we only give a range due to the ambiguity of the phase of f , including the uncertainties from the other fitted parameters and from the lifetimes of charmed baryons. The exceptions in the DCS amplitudes do not affect the fitting very much. Besides, the branching fractions of Λ + c → Σ 0 π + and Σ + π 0 are identical to each other due to the isospin symmetry. From table 1, it is clear that our results are well consistent with the data. It is plausible that the CF and DCS transitions of charm baryons are well expressed by flavor SU(3) symmetry. Besides, in ref. [27], the authors studied charmed baryon decays under the SU(3) symmetry analysis similarly to our work, but including the SCS processes. Their χ 2 is much larger than ours, and their result of B(Λ + c → pπ 0 ) significantly exceeds the experimental upper bound. The predictions on the branching fractions of Λ + c → pK 0 L and those of Ξ +,0 c decays can be tested by experiments in the future.
From table 1, one can find the branching fractions of B c → BK 0 S are obviously different from the B c → BK 0 L ones due to the interference between the CF and DCS amplitudes, which results in measurable K 0 S − K 0 L asymmetries. The results of K 0 S − K 0 L asymmetries, R(B c → BK 0 S,L ), are given in table 2. It is found that the K 0 S − K 0 L asymmetry in Λ + c → pK 0 S,L decay, the promising observable to search for two-body DCS amplitudes of charmed baryons, can reach the order of 10 −2 or even 0.1, within the experimental capability.
The numerical results of the time-integrated CP asymmetries A CP (t 1 τ S t 2 τ L ) (denoted by A CP for simplification) are presented in table 3. There are two solutions of the CP asymmetries for each parameter set. We label the results obtained from eq. (4.6) by S1, and S2 is obtained by flipping the signs of all phase parameters in S1 since the solution with opposite strong phases contributes equivalently to branching fractions that are proportional to the cosine of the strong phases. The measurements in the future, to establish the above CP asymmetries, could discriminate these solutions. In the absence of the DCS contributions, i.e., r f = 0, A CP (B c → BK 0 S ) = A K 0 CP −2Re[ ] ≈ −3.23 × 10 −3 .
The new CP -violation effect A int CP can be revealed by the subtraction of A K 0 CP and the −2r f cos φ cos δ f term in denominator of eq. (3.14) from the total CP asymmetries. The signs of A int CP are opposite between the solutions of S1 and S2 due to its proportion to sin δ f , while the ones of −2r f cos φ cos δ f are the same in solutions of S1 and S2. The denominator D in eq. (3.14) could be obtained from the corresponding K 0 S − K 0 L asymmetries, seen in eq. (3.15). The new CP asymmetry effect, A int CP , is of the order of 10 −4 , while the direct CP asymmetry A dir CP is O(10 −5 ). For example, the range of A int CP (Λ + c → pK 0 S ) is (0.16 ∼ 3.37) × 10 −4 and the one for A dir CP (Λ + c → pK 0 S ) is (0.3 ∼ 6.8) × 10 −5 in solution S1. The direct CP violation are sensitive to new physics which may contribute to the DCS amplitudes with a large weak phase [49]. Thus if the new CP violating effect was determined in experiment, the direct CP violation in charmed baryon decays into neutral kaons can be obtained and used to search for new physics.

Summary
Charmed baryon decays are becoming more intriguing due to the new measurements by Belle and BESIII in recent years. In this work, we investigate the K 0 S − K 0 L asymmetries and CP violation in charmed baryon decays into neutral kaons. Induced by the interference between the Cabibbo-favored and the doubly Cabibbo-suppressed amplitudes, the K 0 S −K 0 L asymmetries can be used to study the DCS amplitudes. As no evidence of two-body DCS process in charmed baryon decays has been found so far, we propose to measure the K 0 S −K 0 L asymmetry in the Λ + c → pK 0 S,L decay mode as a promising method to search for the twobody DCS transition. Besides, a new CP -violation effect is found in charmed baryon decays into neutral kaons, induced by the interference between the CF and DCS amplitudes with the K 0 − K 0 mixing. Once it is determined in experiments, the direct CP asymmetries can be used to search for new physics beyond the Standard Model. A numerical analysis based on SU(3) symmetry is preformed to estimate the values of K 0 S − K 0 L asymmetries and CP violations.