Precise measurements of branching fractions for Ds+\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {\mathrm{D}}_{\mathrm{s}}^{+} $$\end{document} meson decays to two pseudoscalar mesons

We measure the branching fractions for seven Ds+\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {D}_s^{+} $$\end{document} two-body decays to pseudo-scalar mesons, by analyzing data collected at s\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ \sqrt{s} $$\end{document} = 4.178 ∼ 4.226 GeV with the BESIII detector at the BEPCII collider. The branching fractions are determined to beBDs+→K+η'=2.68±0.17±0.17±0.08×10−3,BDs+→η'π+=37.8±0.4±2.1±1.2×10−3,BDs+→K+η=1.62±0.10±0.03±0.05×10−3,BDs+→ηπ+=17.41±0.18±0.27±0.54×10−3,BDs+→K+KS0=15.02±0.10±0.27±0.47×10−3,BDs+→KS0π+=1.109±0.034±0.023±0.035×10−3,BDs+→K+π0=0.748±0.049±0.018±0.035×10−3,\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {\displaystyle \begin{array}{c}\mathcal{B}\left({D}_s^{+}\to {K}^{+}\eta \hbox{'}\right)=\left(2.68\pm 0.17\pm 0.17\pm 0.08\right)\times {10}^{-3},\\ {}\mathcal{B}\left({D}_s^{+}\to \eta \hbox{'}{\pi}^{+}\right)=\left(37.8\pm 0.4\pm 2.1\pm 1.2\right)\times {10}^{-3},\\ {}\mathcal{B}\left({D}_s^{+}\to {K}^{+}\eta \right)=\left(1.62\pm 0.10\pm 0.03\pm 0.05\right)\times {10}^{-3},\\ {}\mathcal{B}\left({D}_s^{+}\to \eta {\pi}^{+}\right)=\left(17.41\pm 0.18\pm 0.27\pm 0.54\right)\times {10}^{-3},\\ {}\mathcal{B}\left({D}_s^{+}\to {K}^{+}{K}_S^0\right)=\left(15.02\pm 0.10\pm 0.27\pm 0.47\right)\times {10}^{-3},\\ {}\mathcal{B}\left({D}_s^{+}\to {K}_S^0{\pi}^{+}\right)=\left(1.109\pm 0.034\pm 0.023\pm 0.035\right)\times {10}^{-3},\\ {}\mathcal{B}\left({D}_s^{+}\to {K}^{+}{\pi}^0\right)=\left(0.748\pm 0.049\pm 0.018\pm 0.035\right)\times {10}^{-3},\end{array}} $$\end{document} where the first uncertainties are statistical, the second are systematic, and the third are from external input branching fraction of the normalization mode Ds+\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ {D}_s^{+} $$\end{document} → K+K−π+. Precision of our measurements is significantly improved compared with that of the current world average values.


Introduction
Among the hadronic decays of the strange-charmed meson D + s , the theoretical treatment based on QCD-inspired models of its decays into two pseudoscalar mesons (D + s → PP ) is the cleanest [1,2]. Precision measurements of these decay rates can provide crucial calibrations to different theoretical models [1][2][3][4][5]. For each decay branching fraction (BF) listed in table 1, the precision of current measurements listed by the Particle Data Group (PDG) [6] is still not good enough to test theoretical models. Hence, more precise and independent measurements are desired to further improve our understanding of QCD dynamics in charm physics.
In 2019, LHCb discovered CP violation in D 0 → π + π − and D 0 → K + K − decays with a significance of 5.3σ [7], providing stringent constraints on theoretical approaches to CP violation in the charm sector [1,4,8]. For the strange-charmed meson D + s , there are theoretical predictions for the CP asymmetries of the singly Cabibbo-suppressed (SCS) decay modes, which rely on the potential effect of SU(3) symmetry breaking [3,9]. However, the current world average results, as shown in table 1, suffer from large uncertainties and are thus insensitive to SU (3) breaking. More precise measurements of the BFs for the SCS modes in D + s → PP will help to explore SU(3) symmetry breaking in D + s decays [3,9]. As a result, more reliable theoretical predictions of CP asymmetries in the D + s SCS hadronic decays can be achieved.
A partial reconstruction technique is adopted: only one D ± s , decaying into the P P mode, is detected along with a soft photon from D * ± s (D * ∓ s ); the other D ∓ s is not used. The BFs are measured relative to the normalization mode D + s → K + K − π + . In the context, charge conjugate modes are always implied, unless explicitly mentioned.

BESIII detector and Monte Carlo simulation
The BESIII detector is a magnetic spectrometer [15] located at BEPCII [16]. The cylindrical core of the BESIII detector consists of a helium-based main drift chamber (MDC), a plastic scintillator time-of-flight system (TOF), and a CsI(Tl) electromagnetic calorimeter (EMC), which are all enclosed in a superconducting solenoidal magnet providing a 1.0 T magnetic field. The solenoid is supported by an octagonal flux-return yoke with resistive plate counter muon tracker modules interleaved with steel. The acceptance of charged particles and photons is 93% over 4π solid angle. The charged-particle momentum resolution at 1 GeV/c is 0.5%, and the ionization energy loss dE/dx resolution is 6% for the electrons from Bhabha scattering. The EMC measures photon energies with a resolution of 2.5% (5%) at 1 GeV in the barrel (end cap) region. The time resolution of the TOF barrel part is 68 ps, while that of the end cap part is 110 ps. The end cap TOF system was upgraded in 2015 with multi-gap resistive plate chamber technology, providing a time resolution of 60 ps [17,18]. Only the 4.226 GeV data was taken before this upgrade.
Simulated data samples, produced with the geant4-based [19] Monte Carlo (MC) package which includes the geometric description of the BESIII detector and the detector response, are used to determine the detection efficiency and to estimate the backgrounds. The simulation includes the beam energy spread and initial state radiation in the e + e − annihilations modeled with the generator kkmc [20,21]. In order to study the backgrounds, generic MC samples consisting of open-charm states, radiative return to J/ψ and ψ(2S), and continuum processes of qq (q = u, d, s), along with Bhabha scattering, µ + µ − , τ + τ − , and γγ events are generated. The known decay modes are modeled with evtgen [22,23] JHEP08(2020)146 using BFs taken from PDG [6], and the remaining unknown decays from the charmonium states are treated with lundcharm [24,25]. Final state radiation (FSR) from charged final state particles is incorporated with the photos package [26]. The signal MC samples of e + e − → D * ± s D ∓ s with a D + s meson decaying to the signal decay modes together with a D − s decaying inclusively are generated with ConExc [27].

Measurement method
In this analysis, a candidate D + s meson is reconstructed by the combination of the detected final-state particles. With current precision, CP violation is negligible, which means the BFs for D + s decays to the mode i + , B i + ≡ B(D + s → i + ), and for D − s decays to the mode i − , B i − , are equal. Therefore, we denote B i + = B i − = B i . The yield, n i , of the observed D + s → i signal events at all six energy points can be written as s is the total number of D * + s D − s pairs produced in all the data samples. For mode i, B i final-state is the combined BF from the i state to the observed final state (those are described in section 4), and ε i is average detection efficiency for the whole data set, which is given as Here, L k is the integrated luminosity, σ k is the observed cross section and ε i k is the detection efficiency at the k-th energy point.
The absolute BF of the normalization mode decay, D + s → K + K − π + , is denoted by B K + K − π + and is taken from PDG [6]. Based on eq. (3.1), the relative BF for the signal mode D + s → i is (3. 3) The absolute BF B i is obtained by

Event selection
Charged tracks are reconstructed from hits in the MDC. Except for the tracks used to reconstruct the K 0 S meson, the distances of closest approach to the interaction point are required to satisfy R xy < 1.0 cm in the xy plane perpendicular to the z direction of the MDC and R z < 10.0 cm along the z direction. The track polar angle θ must satisfy | cos θ| < 0.93. For particle identification (PID) of charged tracks, measurements of dE/dx and the flight time measured by the TOF are combined to form a likelihood L(h) (h = π, K) for each JHEP08(2020)146 hadron hypothesis. Tracks are identified as charged pions when the PID likelihoods of pions are larger than those of kaons, L(π) > L(K), while tracks with L(K) > L(π) are identified as kaons.
Shower clusters with no association to any charged tracks in the EMC crystals will be identified as photon candidates when the following requirements are fulfilled: the measured EMC time is within 0 t 700 ns of the event start time to suppress the electronic noise and showers unrelated to the events; the deposited energy is larger than 25 MeV in the barrel (|cos θ| < 0.80) and larger than 50 MeV in the end cap (0.86 < |cos θ| < 0.92). Additionally, the angle between a photon candidate and the nearest charged track must be larger than 10 • to prevent contamination from hadronic showers.
Candidate K 0 S mesons are reconstructed from two oppositely charged tracks, with no PID requirement; these tracks are required to satisfy the polar angle requirement |cos θ| < 0.93 and R xy < 20 cm. Furthermore, there is usually a detectable displacement before the decay of K 0 S meson due to its relatively long lifetime. Therefore, the decay length and corresponding uncertainty of K 0 S candidates are required to satisfy L/σ L > 2, which suppresses prompt π + π − combinatorial background [28]. The K 0 S meson candidates with an invariant mass M (π + π − ) within the mass window [0.491, 0.505] GeV/c 2 are retained.
For a specific D + s decay mode, the D + s signal candidates are formed by combining all the detected final-state particles. In addition, a radiative photon from the D * ± s decay must be detected. Among all the γD + s combinations in the event, the one with the minimal |∆E| is kept for subsequent analysis only, where ∆E is the difference between the center-of-mass energy E 0 ≡ √ s and the total energy of γD + s D − s in the center-of-mass frame of the e + e − beams Here E D + s and E γ are the energies of reconstructed D + s and γ from D * ± s , respectively. E rec is the energy of the recoiled D − s , calculated using where − → p D + s is the total momentum of the detected D + s , − → p γ is the momentum of the radiative photon γ, and m D − s is the nominal mass of the D − s [6]. For a correctly reconstructed D + s candidate, ∆E is expected to be around zero. Therefore, candidates will be rejected when they fail the requirements of ∆E for each decay mode, as shown in table 2, which correspond to the ±3σ regions of the signal ∆E distributions. To further improve the kinematic resolutions of the final states, a kinematic fit is performed to constrain the recoil mass of the D + s γ, M rec (D + s γ), to the nominal mass of the D − s . According to the kinematic fit, the four momenta of all the final-state particles are updated.  As an example, data for D + s → K + π 0 is shown in figure 1; the two-dimensional distribution of the recoil mass M rec (D + s ) and the invariant mass M (D + s γ) depicts the two resonance structures of the processes. The horizontal band corresponds to e + e − →

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To improve the signal-to-background ratio, we further retain only events lying in the regions of the horizontal or vertical bands defined in table 2.

Signal yield and branching fraction
To extract the signal yields for the signal D + s → PP decay modes and the normalization decay mode, unbinned extended maximum likelihood fits are performed on the M (D + s )

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Decay  Table 3. Summary of the signal yields, average detection efficiencies, relative BFs and absolute BFs of individual signal decay modes. The first uncertainty is statistical, the second is systematic, and the third is external, from the BF of the normalization mode D + s → K + K − π + [6]. The uncertainties on efficiencies are due to the limited MC event statistics.
distributions of the selected candidates in data. In each fit, the probability density function (PDF) is parameterized as the sum of signal and background PDFs. The signal PDF is a template shape formed from the signal MC sample convolved with a Gaussian function to compensate the resolution difference between data and MC simulations. For the more common Cabibbo-favored (CF) decay modes D + s → η π + and the SCS decay D + s → K + π 0 , the Gaussian parameters are left free. For the low-yield SCS decays D + s → K 0 S π + , D + s → K + η and D + s → K + η , the Gaussian parameters are fixed at the values obtained from the corresponding fits to the CF decay modes D + s → K + K 0 S , D + s → ηπ + and D + s → η π + , respectively, since the kaons and pions have almost the same kinematics. According to the background study using inclusive MC samples, peaking backgrounds are present for the modes of D + s → η π + , D + s → K + K 0 S and D + s → K 0 S π + . The peaking backgrounds are modeled in the fit with the MC-determined shape and size. The fractions of the peaking background in the total event yields are estimated to be 2.0%, 1.4% and 1.6% for D + s → η π + , D + s → K + K 0 S and D + s → K 0 S π + , respectively. The non-peaking background components are described with linear functions and second-order Chebychev functions for the CF and SCS decay modes, respectively. The fits are presented in figure 2, and the numerical results of the signal yields are listed in table 3. The relative and absolute BFs, calculated with the average detection efficiencies obtained from the signal MC simulations, are summarized in table 3.

Systematic uncertainty
The sources of systematic uncertainties considered in obtaining the relative BFs include the MC statistics, σ(e + e − → D * + s D − s ) lineshape, shapes of invariant mass distributions for signal and background, peaking background modeling, kinematic fit, ∆E and invariant mass requirements, reconstruction efficiency estimation and quoted BFs. Table 4 summarizes all of these systematic uncertainties. Some correlated uncertainties between the signal decay JHEP08(2020)146 • MC Statistics. Average detection efficiencies are evaluated using MC simulated samples. The uncertainties due to the limited sample sizes, obtained by propagating the statistical uncertainties of the individual efficiencies at different energy points according to eq. (3.2), are assigned as systematic uncertainties.
• σ(e + e − → D * + s D − s ) lineshape. Signal PDFs and detection efficiencies have slight dependencies on the input lineshape of σ(e + e − → D * + s D − s ). To evaluate this uncertainty, different lineshapes are used to estimate the detection efficiencies and data yields. The resulting changes in BFs are taken as systematic uncertainties.
• Signal shape. The uncertainties related to the signal shapes are studied using the decays D + s → K + π 0 , D + s → η π + , D + s → ηπ + and D + s → K + K 0 S . In the nominal analysis, signal shape in the M (D + s ) distribution of the signal candidates is modeled by the signal PDF convolved with a Gaussian function. Double-Gaussian functions are used instead as convolution functions, and the resultant changes of BFs are taken as systematic uncertainties. For the low-yield SCS decays D + s → K 0 S π + , D + s → K + η and D + s → K + η the uncertainties of the corresponding CF modes are used.
• Background shape. In the nominal analysis, the background shapes are described by first-order polynomial functions for the decays D + s → η π + , D + s → ηπ + , D + s → K + K 0 S and D + s → K + K − π + and second-order polynomials for the decays D + s → K + η , D + s → K + η, D + s → K 0 S π + and D + s → K + π 0 . To estimate the uncertainties from the background shapes, higher-order polynomials are considered as alternatives: second-order and third-order, respectively. The resulting changes of the BFs are taken as systematic uncertainties.
• Kinematic fit. High-yield CF decays of D + s → K + K 0 S and D + s → ηπ + are used to study the uncertainty due to the kinematic fit. We perform the analysis without applying the kinematic fit. The differences from the nominal results are taken as systematic uncertainties. For the D + s → K 0 S π + mode the uncertainty from D + s → K + K 0 S is taken while the uncertainty from D + s → ηπ + is assigned to the decays with photons in the final states. • Reconstruction efficiency. We consider the efficiencies of tracking and PID (K ± , π ± ) and the efficiencies of intermediate particles (π 0 , η, K 0 S ) reconstructions, which are studied based on a series of control samples. The K ± and π ± tracking and PID efficiencies are studied using control samples of e + e − → K + K − π + π − , K + K − K + K − , K + K − π + π − π 0 , π + π − π + π − and π + π − π + π − π 0 events [30]. A partial cancellation of the tracking and PID uncertainties in the ratio of the signal modes and the normalization mode is taken into account. The π 0 and η reconstruction efficiencies are evaluated using the double-tag DD hadronic decays D 0 → K − π + , K − π + π + π − ver-susD 0 → K + π − π 0 , K 0 S π 0 [31, 32] and approximating the η behavior as similar to the π 0 . The K 0 S reconstruction efficiency is studied with samples of J/ψ → K * (892) ± K ∓ , K * (892) ± → K 0 S π ± and J/ψ → φK 0 S K ∓ π ± [33]. To account for the different kinematics of the various signal modes, the nominal detection efficiencies are scaled based on event-by-event corrections according to the momentum-dependent efficiency differences between MC simulations and data. The appropriately averaged scaling factors are assigned as the corresponding systematic uncertainties, as given in table 4. Here, the D + s → K + η and D + s → η π + decays suffer from large reconstruction uncertainties due to the low-momentum charged pions and η from η decay.

Summary and discussion
The BFs for D + s → K 0 S π + and D + s → K + π 0 are measured using e + e − collision data collected at √ s = 4.178 ∼ 4.226 GeV in the BESIII experiment. The results obtained in this work are listed in table 3 and can be compared with the results from PDG [6] as well as with theoretical predictions [1,2,4,5] (table 1). Our results are consistent with the PDG values, while the precision is three to five times better than that of previous results. In addition, our results in general agree with the available theoretical calculations [1][2][3][4][5] within about 3σ. However, the discrepancies from our measurements are significant for the model calculations in ref. [1] for the modes D + s → K + η and D + s → K + η, and from the model calculations in ref. [4] for the mode D + s → K + η. Investigating these discrepancies should aid in further developing these QCD-derived models in charm physics.