Resonances in e + e − annihilation near 2 . 2 GeV

J. P. Lees, V. Poireau, V. Tisserand, E. Grauges, A. Palano, G. Eigen, D. N. Brown, Yu. G. Kolomensky, M. Fritsch, H. Koch, T. Schroeder, R. Cheaib, C. Hearty, T. S. Mattison, J. A. McKenna, R. Y. So, V. E. Blinov, A. R. Buzykaev, V. P. Druzhinin , V. B. Golubev, E. A. Kozyrev, E. A. Kravchenko, A. P. Onuchin, S. I. Serednyakov, Yu. I. Skovpen, E. P. Solodov, K. Yu. Todyshev, A. J. Lankford, B. Dey, J. W. Gary, O. Long, A. M. Eisner, W. S. Lockman, W. Panduro Vazquez, D. S. Chao, C. H. Cheng, B. Echenard, K. T. Flood, D. G. Hitlin, J. Kim, Y. Li, T. S. Miyashita, P. Ongmongkolkul, F. C. Porter, M. Röhrken, Z. Huard, B. T. Meadows, B. G. Pushpawela, M. D. Sokoloff, L. Sun, J. G. Smith, S. R. Wagner, D. Bernard, M. Verderi, D. Bettoni, C. Bozzi, R. Calabrese, G. Cibinetto, E. Fioravanti, I. Garzia, E. Luppi, V. Santoro, A. Calcaterra, R. de Sangro, G. Finocchiaro, S. Martellotti, P. Patteri, I. M. Peruzzi, M. Piccolo, M. Rotondo, A. Zallo, S. Passaggio, C. Patrignani, B. J. Shuve, H. M. Lacker, B. Bhuyan, U. Mallik, C. Chen, J. Cochran, S. Prell, A. V. Gritsan, N. Arnaud, M. Davier, F. Le Diberder, A. M. Lutz, G. Wormser, D. J. Lange, D. M. Wright, J. P. Coleman, E. Gabathuler, D. E. Hutchcroft, D. J. Payne, C. Touramanis, A. J. Bevan, F. Di Lodovico, R. Sacco, G. Cowan, Sw. Banerjee, D. N. Brown, C. L. Davis, A. G. Denig, W. Gradl, K. Griessinger, A. Hafner, K. R. Schubert, R. J. Barlow, G. D. Lafferty, R. Cenci, A. Jawahery, D. A. Roberts, R. Cowan, S. H. Robertson, R. M. Seddon, N. Neri, F. Palombo, L. Cremaldi, R. Godang,37,∥ D. J. Summers, P. Taras, G. De Nardo, C. Sciacca, G. Raven, C. P. Jessop, J. M. LoSecco, K. Honscheid, R. Kass, A. Gaz, M. Margoni, M. Posocco, G. Simi, F. Simonetto, R. Stroili, S. Akar, E. Ben-Haim, M. Bomben, G. R. Bonneaud, G. Calderini, J. Chauveau, G. Marchiori, J. Ocariz, M. Biasini, E. Manoni, A. Rossi, G. Batignani, S. Bettarini, M. Carpinelli, G. Casarosa, M. Chrzaszcz, F. Forti, M. A. Giorgi, A. Lusiani, B. Oberhof, E. Paoloni, M. Rama, G. Rizzo, J. J. Walsh, L. Zani, A. J. S. Smith, F. Anulli, R. Faccini, F. Ferrarotto, F. Ferroni, A. Pilloni, G. Piredda, C. Bünger, S. Dittrich, O. Grünberg, M. Heß, T. Leddig, C. Voß, R. Waldi, T. Adye, F. F. Wilson, S. Emery, G. Vasseur, D. Aston, C. Cartaro, M. R. Convery, J. Dorfan, W. Dunwoodie, M. Ebert, R. C. Field, B. G. Fulsom, M. T. Graham, C. Hast, W. R. Innes, P. Kim, D.W. G. S. Leith, S. Luitz, D. B. MacFarlane, D. R. Muller, H. Neal, B. N. Ratcliff, A. Roodman, M. K. Sullivan, J. Va’vra, W. J. Wisniewski, M. V. Purohit, J. R. Wilson, A. Randle-Conde, S. J. Sekula, H. Ahmed, M. Bellis, P. R. Burchat, E. M. T. Puccio, M. S. Alam, J. A. Ernst, R. Gorodeisky, N. Guttman, D. R. Peimer, A. Soffer, S. M. Spanier, J. L. Ritchie, R. F. Schwitters, J. M. Izen, X. C. Lou, F. Bianchi, F. De Mori, A. Filippi, D. Gamba, L. Lanceri, L. Vitale, F. Martinez-Vidal, A. Oyanguren, J. Albert, A. Beaulieu, F. U. Bernlochner, G. J. King, R. Kowalewski, T. Lueck, I. M. Nugent, J. M. Roney, R. J. Sobie, N. Tasneem, T. J. Gershon, P. F. Harrison, T. E. Latham, R. Prepost, and S. L. Wu


I. INTRODUCTION
Recently, a precise measurement of the e þ e − → K þ K − cross section in the center-of-mass (c.m.) energy range E ¼ 2.00-3.08 GeV was performed by the BESIII Collaboration [1]. In this cross section, a clear interference pattern was observed near 2.2 GeV. To explain this pattern, BESIII inferred the existence of a resonance with a mass of 2239AE7AE11MeV=c 2 and a width of 140 AE 12 AE 21 MeV. In the Particle Data Group (PDG) table [2] there are two vector resonances with a mass near 2.2 GeV=c 2 : ϕð2170Þ and ρð2150Þ. The first is observed in three reactions: e þ e − →ϕð2170Þ [3,4], J=ψ →ηϕð2170Þ [5,6], and e þ e − → ηϕð2170Þ [7], but only in the decay mode ϕð2170Þ → ϕð1020Þf 0 ð980Þ. As shown in Ref. [1], the parameters of the resonance structure observed in the e þ e − → K þ K − cross section differ from the ϕð2170Þ PDG parameters by more than 3σ in mass and more than 2σ in width. The isovector resonance ρð2150Þ is not well established. The PDG lists three e þ e − annihilation processes in which evidence for its existence is seen: e þ e − → f 1 ð1275Þπ þ π − , e þ e − → η 0 π þ π − , and e þ e − → π þ π − . In the first two reactions, wide (Γ ∼ 300 MeV) resonancelike structures are observed near the reaction thresholds [8]. A completely different structure is seen in the third process. A resonance with mass and width 2254 AE 22 MeV=c 2 and 109 AE 76 MeV, respectively, is needed to describe the interference pattern in the e þ e − → π þ π − cross section [9]. Note that the parameters of this resonance are very similar to those mentioned above for the e þ e − → K þ K − reaction from BESIII.
Any resonance in the e þ e − → K þ K − cross section should also be present in e þ e − → K S K L . The most precise data on this reaction near 2 GeV were obtained by the BABAR Collaboration [10]. In this previous work, the e þ e − → K S K L cross section was measured up to 2.2 GeV. Above 2 GeV, the cross section was found to be consistent with zero within the statistical uncertainties of around 20 pb. In the present work we expand the energy region of the BABAR K S K L measurement up to 2.5 GeV. The new K S K L measurements, in conjunction with previous BABAR results for other exclusive e þ e − processes, are used to investigate the nature of the structure observed by BESIII in e þ e − → K þ K − .

II. FIT TO THE BESIII AND BABAR
e + e − → K + K − DATA In Fig. 1 we show BESIII [1] and BABAR [11] data on the dressed Born cross section for the process e þ e − → K þ K − in the energy region of interest. The dressed cross section used to obtain resonance parameters is calculated from the bare cross section (σ b ) listed in Refs. [1,11] where R VP is the factor taking into account the vacuum polarization correction, while C FS is the final-state correction (see, e.g., Ref. [12]). The latter, in particular, takes into account extra photon radiation from the final state. In the energy region of interest, 2.00-2.5 GeV, R VP ≈ 1.04 and C FS ¼ 1.008. The BESIII and BABAR data on the dressed e þ e − → K þ K − cross section are fitted by a coherent sum of resonant and nonresonant contributions Þ is the Breit-Wigner function describing the resonant amplitude, M R , Γ R , and σ R are the resonance mass, width, and peak cross section, PðEÞ is a second-order polynomial describing the nonresonant amplitude, and φ is the relative phase between the resonant and nonresonant amplitudes. The fit result is shown in Fig. 1. The fit yields χ 2 =ν ¼ 55.8=40 (Pðχ 2 Þ ¼ 5%) and the fit parameters are listed in Table I.
The systematic uncertainties in the resonance parameters come mainly from uncertainties in the description of the resonance and nonresonance shapes. The uncertainty due to the absolute c.m. energy calibration is negligible [1,11]. For the signal shape we study the effect of the energydependent width assuming that the main resonance decay mode is either K þ K − or ηρ. We also use another parametrization of the nonresonance amplitude, in which the main energy dependence is given by the function a=ðE 2 − b 2 Þ inspired by the vector-meson dominance model, where a and b are fitted parameters, while small deviations from the main dependence are described by a quadratic polynomial. The nonresonance amplitude may have an energydependent imaginary part originating from vector resonances lying below 2 GeV. Using the results of Ref. [13], we estimate that its fraction reaches 10% at 2 GeV and decreases to 5% at 2.5 GeV. To study the effect of the imaginary parts, we multiply the function PðEÞ in Eq. (1) by a factor of 1 AE iGðEÞ, where GðEÞ is a linear function decreasing from 0.05-0.15 at E ¼ 2 GeV to zero at 2.5 GeV. The deviations from the nominal parameter values listed in Table I are taken as the estimates of the systematic uncertainties given in Table I. The systematic uncertainty in the parameter σ R includes also the correlated systematic uncertainty in the e þ e − → K þ K − cross section, which is 2.5% (6%) for the BESIII (BABAR) data.
Our values for the resonance mass and width are close to the values 2239 AE 7 AE 11 MeV=c 2 and 140 AE 12 AE 21 MeV obtained in Ref. [1]. We also perform the fit to the BABAR data only. The resulting parameters are The resonance significance in the BABAR data estimated from the χ 2 difference for the fits with and without the resonance contribution is 3.5σ.
The data analysis presented in this paper is based on methods developed for the measurement of the e þ e − → K S K L cross section in Ref. [10]. The data set, with an integrated luminosity of 469 fb −1 [14], was collected with the BABAR detector [15] at the SLAC PEP-II asymmetric-energy e þ e − storage ring at the ϒð4SÞ resonance and 40 MeV below this resonance. The initial-stateradiation (ISR) technique is used, in which the cross section for the process e þ e − → K S K L is determined from the K S K L invariant mass spectrum measured in the reaction e þ e − → K S K L γ.
The selection criteria for e þ e − → K S K L γ events are described in detail in Ref. [10]. We require the detection of all the final-state particles. The ISR photon candidate must have an energy in the c.m. frame greater than 3 GeV. The K S candidate is reconstructed using the K S → π þ π − decay mode. Two oppositely charged tracks not identified as electrons are fitted to a common vertex. The distance between the reconstructed K S decay vertex and the beam axis must be in the range from 0.2 to 40.0 cm. The cosine of the angle between a vector from the beam interaction point to the K S vertex and the K S momentum in the plane transverse to the beam axis is required to be larger than 0.9992. The invariant mass of the K S candidate must be in the range 0.482-0.512 GeV=c 2 . The K L candidate is a m(K + K -) (GeV/c 2 ) σ(e  cluster in the calorimeter with energy deposition greater than 0.2 GeV. To suppress background, we also require the event to not contain extra charged tracks originating from the interaction region or extra photons with energy larger than 0.5 GeV. The ISR photon, K S , and K L candidates are subjected to a three-constraint kinematic fit to the e þ e − → K S K L γ hypothesis with the requirement of energy and momentum balance. Only the angular information is used in the fit for the K L candidate. If there are several K L candidates in an event, the K S K L γ combination giving the smallest χ 2 value is retained. The particle parameters after the kinematic fit are used to calculate the K S K L invariant mass mðK S K L Þ, which is required to satisfy 1.06 < mðK S K L Þ < 2.5 GeV=c 2 . The χ 2 distribution from the fit for the selected events is shown in Fig. 2 in comparison with the simulated signal and background distributions. The background is dominated by the ISR processes e þ e − → K S K L π 0 γ, K S K L ηγ, and K S K L π 0 π 0 γ. The condition χ 2 < 10 is applied to select signal events. The control region 10 < χ 2 < 20 is used to estimate and subtract background. The numbers of signal (N s ) and background (N b ) events in the signal region (χ 2 < 10) are determined as where N 1 and N 2 are the numbers of selected data events in the signal and control regions, and a ¼ 0.20 AE 0.01 and b ¼ 0.87 AE 0.09 are the N 2 =N 1 ratios for signal and background, respectively. The value of the coefficient a is determined from the simulated signal χ 2 distribution. For the mass region of interest 2.0 < mðK S K L Þ < 2.5 GeV=c 2 , where the number of signal events is small, the aN s term in the expression for N b is negligible. The coefficient b is determined in two ways: either using background simulation, or from the difference between the data and simulated signal distributions in Fig. 2. The signal distribution is normalized to the number of data events with χ 2 < 3 after subtraction of the background estimated from simulation. The average of the two b values is quoted above. Their difference (10%) is taken as an estimate of the systematic uncertainty in b. As shown in Ref. [10], the background mðK S K L Þ distribution obtained using Eq. (2) is found to be in reasonable agreement with the same distribution obtained from simulation.
The background estimated from the control region decreases monotonically with increasing mðK S K L Þ and is well approximated by a smooth function. Figure 3 shows the mðK S K L Þ distribution for data events from the signal region. The curve represents the estimated background distribution.
The uncertainty in the background is 12%, which includes the 10% uncertainty in the parameter b in Eq. (2) and a 6% uncertainty in the background approximation. We do not see a significant signal of K S K L events over background. The e þ e − → K S K L cross section in the mass region 1.96 < mðK S K L Þ < 2.56 GeV=c 2 obtained from the mass spectrum in Fig. 3 after background subtraction is shown in Fig. 4 (left). The details on the detection efficiency and ISR luminosity can be found in Ref. [10]. The numerical values of the e þ e − → K S K L cross section, with statistical and systematic uncertainties, are listed in Table II. The systematic uncertainties arise mainly from the background subtraction and are fully correlated between different mðK S K L Þ intervals. A fit to the cross section data with a constant yields χ 2 =ν ¼ 11.7=13, where ν is the number of degrees of freedom. The average value of the e þ e − → K S K L cross section between 1.98 and 2.54 GeV=c 2 is found to be (4 AE 5 AE 5) pb, which is therefore consistent with zero. The dashed curve in Fig. 4 (left) represents the cross section for the resonance with the parameters listed in Table I. Formally, from the χ 2 difference between the two hypotheses in Fig. 4 (left) the resonance interpretation can be excluded at 2.3σ. However, possible destructive interference between the resonant and nonresonant e þ e − → K S K L amplitudes may significantly weaken this constraint. We also must take into account the uncertainty in the background subtraction and the statistical uncertainty in the resonance cross section obtained from the fit to the e þ e − → K þ K − data. To do this we fit the mass spectrum shown in Fig. 3 with a sum of signal and background distributions. The background distribution shown in Fig. 3 is multiplied by a scale factor r bkg , which is allowed to vary within a 12% uncertainty around unity. The signal cross section is described by Eq. (1) with a constant nonresonant amplitude PðEÞ ¼ ffiffiffiffiffiffiffi ffi σ NR p and the parameter σ R varied around the value listed in Table I. From the fit we determine σ NR and φ. The result of the fit is shown by the curve in Fig. 4 (right). The fitted value of the parameter r bkg is 0.94. Therefore, the points in Fig. 4 (right) lie slightly higher than those in Fig. 4 (left). The fit yields χ 2 =ν ¼ 11.0=12 and the following values of parameters: We conclude that the BABAR data on the e þ e − → K S K L cross section do not exclude the existence of the resonance with the parameters listed in Table I Table I. Right panel: The curve is the result of the fit to the e þ e − → K S K L data with a coherent sum of a resonant amplitude with the parameters listed in Table I and a nonresonant constant amplitude. The points with error bars represent the data following subtraction of the background, which has been scaled by a factor of 0.94 (see text). IV. SIMULTANEOUS FIT TO THE e + e − → K + K − , π + π − , AND π + π − η DATA WITH AN ISOVECTOR RESONANCE As discussed in the Introduction, the mass and width of the resonance observed in the process e þ e − → K þ K − near 2.2 GeV are close to the parameters of the state seen in the e þ e − → π þ π − cross section measured by BABAR [9]. The latter cross section in the energy range 2.00-2.55 GeV is shown in Fig. 5 (left). An interference pattern in the energy region near 2.25 GeV is also seen in the energy dependence of the e þ e − → π þ π − η cross section recently measured by BABAR [16] and shown in Fig. 5 (right). We perform a simultaneous fit to the e þ e − → π þ π − and π þ π − η data. The cross sections are described by formulas similar to Eq. (1). For the π þ π − η channel, the phase space factor βðEÞ 3 =βðM R Þ 3 in Eq. (1) is replaced by the factor p η ðEÞ 3 = p η ðM R Þ 3 M R =E [17], where p η is the η-meson momentum calculated in the model of the ρð770Þη intermediate state.
The nonresonant amplitude is described by the function a=ðE 2 − b 2 Þ inspired by the vector-meson dominance model. The ten fitted parameters are the mass (M R ) and width (Γ R ) of the resonance, the peak cross sections [σðe þ e − → R → π þ π − Þ and σðe þ e − → R → π þ π − ηÞ], and a, b, and φ for the two channels. The result of the fit is shown in Fig. 5 by the solid curves. The fit parameters obtained are listed in the second column of Table III. The fit yields χ 2 =ν ¼ 14.0=12 (Pðχ 2 Þ ¼ 0.30). The significance of the resonance calculated from the difference in χ 2 with and without the resonance contributions is 4.6σ. The systematic uncertainties in the resonance parameters are determined as described in Sec. II.
147 AE 30 AE 10 188 AE 19 AE 9 φðe þ e − → π þ π − ηÞ (deg) 217 AE 24 AE 9 251 AE 15 AE 9 χ 2 =ν 13.96=12 17.2=14 section is parametrized as described in Sec. II. The fit parameters obtained are listed in the third column of Table III. Since the e þ e − → K þ K − data are statistically more accurate than the π þ π − or π þ π − η data, the fitted resonance mass, width, and σðe þ e − → R → K þ K − Þ are similar to those (Table I) obtained in the fit to the K þ K − data alone. The results of the fit for e þ e − → π þ π − and π þ π − η cross sections are shown in Fig. 5 by the dashed curves. The χ 2 =ν calculated using the π þ π − and π þ π − η data is 17.2=14 (Pðχ 2 Þ ¼ 0.25). We conclude that it is very likely that the interference patterns observed in the three cross sections discussed above are manifestations of the same isovector resonance, ρð2230Þ. It is interesting to note that the decay rates of this state to K þ K − , π þ π − , and π þ π − η are all similar.

V. TWO-RESONANCE FIT
The isovector state discussed in the previous section is expected to have an ω-like isoscalar partner with a similar mass. An indication of an isoscalar resonance structure near 2.25 GeV is seen in the e þ e − → ωπ þ π − and e þ e − → ωπ 0 π 0 cross sections measured by BABAR [8,18]. The energy dependence of the total e þ e − → ωππ (ωπ þ π − þ ωπ 0 π 0 ) cross section in the energy region of interest is shown in Fig. 6. It is fitted by a coherent sum of resonant and nonresonant contributions. We assume that the process e þ e − → ωππ proceeds via the ωf 0 ð500Þ intermediate state. Therefore, the factor βðEÞ 3 =βðM R Þ 3 in Eq. (1) is replaced by the s-wave phase-space factor p ω ðEÞ=p ω ðM R Þ, where p ω is the ω-meson momentum in e þ e − → ωf 0 ð500Þ. It should be noted that the phase-space factor for the other possible intermediate state, b 1 ð1235Þπ, has a similar energy dependence in the energy region of interest. The nonresonant amplitude is described by the function a=ðE 2 − b 2 Þ. The fit yields χ 2 =ν ¼ 6.8=6. The result of the fit is shown in Fig. 6 by the solid curve. The fitted resonance mass (2265 AE 20 MeV=c 2 ) and width (75 þ125 −27 MeV) are similar to the parameters of the isovector state in Table III. Since different intermediate mechanisms (e.g., ωf 0 and b 1 π) contribute to the ωππ final state, the resonant and nonresonant amplitudes may be not fully coherent. Inclusion in the fit of an incoherent contribution describing up to 50% of the nonresonant cross section has an insignificant impact on the fitted resonance mass and width. The dashed curve in Fig. 6 is the result of the fit to data with a second-order polynomial. The χ 2 =ν for this fit is 18.1=9. From the χ 2 difference between the two fits we estimate that the significance of the resonance signal in the e þ e − → ωππ cross section is 2.6σ.
From isospin invariance, the isovector amplitude enters the e þ e − → K þ K − and e þ e − → K S K L amplitudes with the opposite sign (in contrast to the isoscalar case) [19]: The quark model predicts [19] that the isoscalar amplitude related to the ω-like resonance is one-third the amplitude of the corresponding ρ-like state and that these amplitudes have the same sign in the e þ e − → K þ K − channel. If the ρand ω-like resonances have similar masses and widths, we expect the resonance amplitude in the e þ e − → K S K L reaction to be about two times smaller than that in e þ e − → K þ K − . This weakens the constraints on the nonresonant e þ e − → K S K L cross sections and the interference phase, relation (3), obtained in the fit to the e þ e − → K S K L data in Sec. [10]. Repeating this fit with the resonance amplitude smaller by a factor of two, we obtain χ 2 =ν ¼ 10.6=12 and the parameters The fit with the zero nonresonant cross section also has an acceptable χ 2 value, 12.1=14. We conclude that the tworesonance fit allows a simultaneous description of the e þ e − → K þ K − and e þ e − → K S K L data without strong constraints on the interference parameters in the e þ e − → K S K L channel. Finally, we fit the e þ e − → K þ K − , e þ e − → π þ π − , and e þ e − → π þ π − η data using the model described in Sec. IV with an additional contribution from the ϕð2170Þ resonance. The ϕð2170Þ mass and width are fixed at their PDG values [2]. The inclusion of the ϕð2170Þ has an insignificant impact on the quality of the fit. The fitted value of the ϕð2170Þ peak cross section is found to be consistent with zero, 0.8 þ2. 9 −0.8 pb.

VI. SUMMARY
In this paper, we present measurements of the e þ e − → K S K L cross section in the center-of-mass range from 1.98 to 2.54 GeV. The measured cross section is consistent with zero and does not exhibit evidence for a resonance structure. The K S K L data are analyzed in conjunction with BESIII [1] and BABAR [11] data on the e þ e − → K þ K − cross section, and with BABAR data on the e þ e − → π þ π − [9], π þ π − η [16], ωπ þ π − þ ωπ 0 π 0 [8,18] cross sections to examine properties and better elucidate the nature of the resonance structure observed by BESIII in the e þ e − → K þ K − cross section near 2.25 GeV [1].
The interference patterns seen in the e þ e − → π þ π − and e þ e − → π þ π − η data near 2.25 GeV provide 4.6σ evidence for the existence of the isovector resonance ρð2230Þ. Its mass and width are consistent with the parameters of the resonance observed in the e þ e − → K þ K − channel. All three cross sections are well described by a model with ρð2230Þ mass and width M ¼ 2232 AE 8 AE 9 MeV=c 2 and Γ ¼ 133 AE 14 AE 4 MeV.
Any resonance in the e þ e − → K þ K − cross section should also be manifest in the e þ e − → K S K L cross section. The BABAR data on the e þ e − → K S K L cross section do not exclude the existence of the ρð2230Þ resonance, but strongly restrict the possible range of allowed values of the relative phase between the resonant and nonresonant e þ e − → K S K L amplitudes. This restriction may be significantly weakened by inclusion in the fit of an additional isoscalar resonance with a nearby mass. An indication of such a resonance with 2.6σ significance is seen in the e þ e − → ωππ cross section.
Further study of the resonance structures near 2.25 GeV can be performed at the BESIII experiment, where the cross sections for e þ e − → π þ π − η, ωπ þ π − , ωπ 0 π 0 and other exclusive processes in the energy range between 2 and 2.5 GeV may be measured with high accuracy.