Measurement of the inclusive charm cross section at 4.03 GeV and 4.14 GeV

and 4.14 GeV has been measured with the Beijing Spectrometer. The measurement was made using 22.3 pb 2 1 of e 1 e 2 data collected at 4.03 GeV and 1.5 pb 2 1 of e 1 e 2 data collected at 4.14 GeV. Inclusive observed cross sections for the production of charged and neutral D mesons and momentum spectra are presented. Observed cross sections were radiatively corrected to obtain tree level cross sections. Measurements of the total hadronic cross section are obtained from the charmed meson cross section and an extrapolation of results from below the charm threshold.


I. INTRODUCTION
The hadronic cross section of e ϩ e Ϫ at all energies is needed to calculate the effects of vacuum polarization on parameters of the standard model. The energy region which contributes the largest uncertainty is the charm threshold region where the hadronic cross section has only been measured with an accuracy of 15-20% ͓1͔. Traditionally, hadron is measured by counting hadronic events. This method re-quires a detailed understanding of trigger conditions, the efficiency of hadronic event selection criteria, and a subtraction of two photon events and other backgrounds. An alternative is measuring charm and adding this to an extrapolation of the u,d,s contribution from the region below charm threshold. The charmed mesons used in this study are the D 0 and D ϩ . The D s cross sections are taken from earlier works. There is no evidence for continuum charmonium production ͓2͔. The charm counting method is intrinsically less sensitive to trigger conditions, beam-related backgrounds, and two photon backgrounds due to the distinctive topology of charmed meson events. *Deceased. PHYSICAL REVIEW D, VOLUME 62, 012002 0556-2821/2000/62͑1͒/012002͑8͒/$15.00 ©2000 The American Physical Society 62 012002-1

II. DATA SELECTION
The data used for this analysis were accumulated with the Beijing Spectrometer ͓3͔; the total integrated luminosity at 4.03 ͑4.14͒ GeV was 22.3 ͑1.5͒ pb Ϫ1 . Candidate tracks were required to have a good track fit passing within 1.5 cm of the collision point in R and 15 cm in z, and satisfying ͉cos ͉ Ͻ0.85. Particle identification was provided by an array of time of flight ͑TOF͒ scintillation counters and specific ionization measurements in the drift chamber used for charged particle tracking (dE/dx). For pions, consistency ͓CL() Ͼ0.1%͔ and loose electron rejection ͓L /(L ϩL e )Ͼ0.2͔ were required, where L X is the likelihood for hypothesis X. Kaon identification required consistency ͓CL(K)Ͼ0.1%͔, pion rejection ͓L K /(L K ϩL )Ͼ0.5͔ and loose electron rejection ͓L K /(L K ϩL e )Ͼ0.2͔. Multiple counting of D 0 candidates was removed by positively identifying pions using the selection ͓L K /(L K ϩL )Ͻ0.5͔. Muons are rejected using a momentum dependent criteria based on track penetration into the muon detector.

III. D 0 AND D ¿ SIGNAL
Inclusive K Ϫ ϩ and K Ϫ ϩ ϩ invariant mass distributions are shown in Figs. 1 and 2 for 4.03 and 4.14 GeV, respectively. ͑Here and throughout this paper, reference to a state also implies its charge conjugate state.͒ Each histogram was fit to a function which included a Gaussian signal plus a background function. For the K distributions ͓Figs. 1͑a͒ and 2͑a͔͒, the background function consisted of a Gaussian centered at 1.60 GeV to account for the contribution to the K spectrum from D 0 →K 0 decays plus a third order polynomial background. For the K distributions ͓Figs. 1͑b͒ and 2͑b͔͒, the background function consisted of a third order polynomial. The number of signal events in each mode is given in Table I.
The momentum spectra of D candidates with a mass between 1.81 and 1.91 GeV is presented in Fig. 3  In addition, a small low momentum tail on each structure is expected due to initial state radiation. The background shape under the momentum spectrum is not flat, making a direct subtraction difficult.

IV. CROSS SECTION
If the reconstruction efficiency for D mesons were constant with respect to momentum, the observed cross section could be determined using where N(signal) is the number of signal events, ⑀ is the efficiency, B is the branching fraction of the D meson to a decay mode and L is the luminosity. However, Monte Carlo studies show some momentum dependence to the reconstruc- tion efficiency ͑Fig. 5͒. In order to measure the cross section, the momentum spectrum for D 0 and D ϩ mesons from 50 to 850 ͑110 to 1030͒ MeV was divided into 20 ͑40͒ MeV slices for 4.03 ͑4.14͒ GeV data. For each momentum slice, the invariant mass distribution was fit with a Gaussian plus a polynomial background. The central value of the Gaussian was fixed at the nominal D mass; the width was fixed to a momentum dependent value determined by a fit to a coarser slicing of the data ͑Fig. 6͒. The differential cross section with respect to momentum for this data is shown in Figs. 7 and 8 for 4.03 and 4.14 GeV, respectively. The cross section times branching fractions of D 0 and D ϩ mesons and cross sections calculated using the branching fractions of Ref. ͓4͔ are shown in Table II. The •B values from this measurement are compatible with previous measurements by Mark I ͓5,6͔ and Mark II ͓7͔ as shown in Fig. 9.

V. CORRECTIONS FOR INITIAL STATE RADIATION
The tree level cross sections for charm at ͱsϭ4.03 GeV and ͱsϭ4.14 GeV were obtained by correcting the observed cross section for the effects of initial state radiation ͑ISR͒. The ISR correction is dependent on the cross section for all energies less than the nominal energy. Since these measurements were performed only at two energies, some theoretical modeling of the cross section distribution was required. Two different theoretical predictions for these cross sections were used in this analysis, the coupled channel model ͓8͔, and a P-wave phase space formalism. The models provide predictions for B,i (s eff ), the tree level ͑Born͒ cross section as a function of the effective center of mass energy squared for The effective center of mass energy squared is given by where k•E beam is the energy of radiated photons and s nom is the nominal center of mass energy squared. The tree level cross sections are convoluted with a sampling function f (k,s nom ) that represents a first order calculation of the effective luminosity for radiated photons in a two body radiation model ͓9͔, giving the observed cross section at s nom :

͑3͒
The vacuum polarization correction (1ϩ␦ VP ) includes both leptonic and hadronic terms. It varies from charm threshold to 4.14 GeV by less than Ϯ2%. It is treated as a constant with the value ͑ 1ϩ␦ VP ͒ϭ1.047Ϯ0.024 ͑4͒ FIG. 8. The differential production cross section of ͑a͒ e ϩ e Ϫ →D 0 X and ͑b͒ e ϩ e Ϫ →D ϩ X versus the momentum of the reconstructed D at E c.m. ϭ4.14 GeV. ͱsϭ4.03 GeV ͱsϭ4.14 GeV The D* 0 and D* ϩ branching fractions are used to calculate N D 0 ,i and N D ϩ ,i , the mean number of D 0 and D ϩ per production mode i event. The N D 0 ,i and N D ϩ ,i values are used to weight the ISR correction for each mode to obtain the ISR correction averaged over all production modes: This procedure results in the corrections shown in Fig. 10. Since neither method models the data precisely, and the two models vary differently with energy, a systematic uncertainty is assigned to be one half the rms difference between the two models over the energy range 3.9 GeV to 4.2 GeV excluding the region from 4.021 to 4.027 where the coupled channel model DD cross section is tiny, causing the ISR correction to diverge. The corrections for initial state radiation at ͱs ϭ4.03 GeV and ͱsϭ4.14 GeV are 4.03 GeV: g D 0ϭ 0.67Ϯ0.05, ͑8͒ 4.14 GeV: g D 0ϭ 0.83Ϯ0.06, ͑10͒ g D ϩϭ 0.84Ϯ0.06. ͑11͒ The ISR correction for D s mesons was calculated using the coupled channel model and the same P-wave phase space formalism. Figure 11 shows a prediction for the tree level cross section of D s and D s * , the observed cross section of D s and D s * , the fraction of D s mesons from direct production, and the fraction of D s mesons from D s * decays. Figure 10͑c͒ shows the ISR correction for D s mesons. The ISR contribution to the systematic error for D s production is taken as one half the rms difference between the two models: 4.03 GeV: g D s ϭ0.73Ϯ0.04, ͑12͒ 4.14 GeV: g D s ϭ0.78Ϯ0.05. ͑13͒ The ISR and vacuum polarization corrections are applied to the observed D 0 and D ϩ cross sections found in Table II to obtain the tree level cross section for D 0 and D ϩ at 4.03 GeV and 4.14 GeV as shown below: 4.03 GeV: D 0ϩ D 0ϭ 19.9Ϯ0.6Ϯ2.3 nb, ͑14͒ D ϩϩ D Ϫϭ 6.5Ϯ0.2Ϯ0.8 nb, ͑15͒ 4.14 GeV: D 0ϩ D 0ϭ 9.3Ϯ2.1Ϯ1.1 nb, ͑16͒

VI. SYSTEMATICS
Several systematic checks were performed. The numbers of signal events in the distributions shown in Figs. 1 and 2 were compared to the sum of signal events from each momentum slice as shown in Table III. Good agreement for the 4.03 GeV data validates the slicing technique. For the 4.14 GeV data set, which is much smaller, the agreement is poorer. This could be due to statistical fluctuations.
The analysis was repeated using wrong sign combinations (K ϩ ϩ ,K ϩ ϩ Ϫ ) to explore systematic bias from the slicing and fitting procedure. As expected, the structures that are so evident in the right sign spectra are absent in the wrong sign spectra ͑Fig. 12͒. There is, however, a small excess when the K Ϫ Ϫ ϩ spectrum is integrated: Both the data and the charged Monte Carlo ͑MC͒ simulation show a small excess that was not present in neutral decays. A much larger MC study would be required to prove whether the source is procedural, or if there is a small feed down FIG. 11. ͑a͒ The tree level cross section for D s mesons. ͑b͒ The tree level cross section for D s * mesons. ͑c͒ The observed cross section for D s mesons. ͑d͒ The observed cross section for D s * mesons. The solid curve was obtained using the coupled channel model. The dashed line was obtained using the p-wave phase space formalism.
FIG. 12. The differential production cross section for wrong sign combinations. ͱsϭ4.03 GeV ͱsϭ4.14 GeV Inclusive D Sum of slices Inclusive D Sum of slices from right sign channels into the wrong sign analysis. If the source of the excess is procedural, the MC efficiency calculation should correct for the effect in the data. In either case, no correction is required. Systematic errors arising from the choice of parameters were evaluated by repeating the analyses using different bin sizes, fitting ranges, mass resolutions, and background function shapes. Electron particle identification dominates the integrated luminosity uncertainty as determined from wide angle Bhabha scattering events. The uncertainty is evaluated by comparing samples selected independently using dE/dx and the barrel shower counter. In addition there are systematic errors due to the uncertainties in the Monte Carlodetermined reconstruction efficiency, errors in the charmed meson branching fractions, and the uncertainties in the evaluation of the ISR correction scheme as discussed above. Magnitudes of these systematic uncertainties are shown in Table IV.
Sources of systematic uncertainty are segregated into components that are common or independent for D 0 , D ϩ , and D S measurements. The common components are the integrated luminosity measurement, the ISR correction, the vacuum polarization correction, and a portion of the D branching fraction uncertainties. Since the absolute branching fraction scale for D ϩ mesons depends on the D 0 branching fraction scale, the total percentage uncertainty for D ϩ branching fraction ͑6.7%͒ is split into a common component that matches the percentage uncertainty for the D 0 branching fraction ͑2.3%͒ and an independent component ͑6.2%͒. All other systematic uncertainties are treated as independent and added in quadrature. Values are found in Table IV. The total observed D 0 and D ϩ cross sections are shown in Table II. Tree level D 0 and D ϩ cross sections are shown in Table V.

VII. TOTAL INCLUSIVE CHARM CROSS SECTION
Since all D mesons are produced in pairs, the tree level nonstrange D cross sections are 4.03 GeV: ͑DD X ͒ϭ13.2Ϯ0.3Ϯ1.4 nb, ͑20͒ 4.14 GeV: ͑DD X ͒ϭ5.6Ϯ1.1Ϯ0.6 nb. ͑21͒ Adding the tree level D cross sections to the tree level D s cross sections gives the total tree level charm cross section: 4.03 GeV: charm ϭ13.6Ϯ0.3Ϯ1.5 nb, ͑22͒ 4.14 GeV: charm ϭ6.4Ϯ1.2Ϯ0.7 nb. ͑23͒ These results are compared to coupled channel model predictions in Table V.

VIII. MEASUREMENT OF R D AND R
A measurement of R D is obtained by dividing 2ϫ charm by the QED prediction for the tree level muon pair cross section ͑e ϩ e Ϫ → ϩ Ϫ ͒ϭ 86.8 nb s͑GeV͒ 2 , ͑24͒ giving 4.03 GeV: R D ϭ5.10Ϯ0.12Ϯ0.55, ͑25͒ 4.14 GeV: R D ϭ2.53Ϯ0.46Ϯ0.27. ͑26͒  The contribution to R in the charm threshold region from the light quarks, R uds is estimated to be 2.5Ϯ0.25 ͓7͔. This value was compiled from an average of measurements of R below charm threshold ͓12-14͔. The theoretical expectation is that R uds is approximately independent of center of mass energy in this region. The value of R is evaluated using RϭR D /2 ϩR uds giving 4.03 GeV: Rϭ5.05Ϯ0.06Ϯ0.37, ͑27͒ 4.14 GeV: Rϭ3.76Ϯ0. 23Ϯ0.28. ͑28͒ This measurement is more precise, but compatible with previous R measurements ͓12,14͔ using the total cross section method shown in Figs. 13͑a͒ and 13͑b͒ and a previous measurement ͓7͔ employing a similar R D technique shown in Fig. 13͑c͒. Charm-counting complements direct R measurements since the two methods feature different systematic uncertainties.