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1.
Thee + e ?K + K ? cross section has been measured from about 750 events in the energy interval \(1350 \leqq \sqrt s \leqq 2400 MeV\) with the DM2 detector at DCI. TheK ± form factor |F F ±| cannot be explained by the ρ, ω, ? and ρ′(1600). An additional resonant amplitude at 1650 MeV has to be added as suggested by a previous experiment.  相似文献   

2.
《Physics letters. [Part B]》1987,184(4):410-416
We calculate the total and differential cross sections for the process e+e→W+W including the effects of the extra Z-boson coming from the E8⊗E8 superstring. It is pointed out that the observation of the total and differential cross sections can determine the relative sign of the Weinberg angle τw and the mixing angle τe between Z'0 and Z E.  相似文献   

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Using recently published, high-precision π + π ? cross section data by the BABAR experiment from the analysis of e + e ? events with high-energy photon radiation in the initial state, we reevaluate the lowest order hadronic contribution $(a_{\mu}^{\mathrm{had},\mathrm{LO}})$ to the anomalous magnetic moment of the muon. We employ newly developed software featuring improved data interpolation and averaging, more accurate error propagation and systematic validation. With the new data, the discrepancy between the e + e ?- and τ-based results for the dominant two-pion mode reduces from previously 2.4σ to 1.5σ in the dispersion integral, though significant local discrepancies in the spectra persist. We obtain for the e + e ?-based evaluation $a_{\mu}^{\mathrm{had},\mathrm{LO}}=(695.5\pm4.1)\times 10^{-10}$ , where the error accounts for all sources. The full Standard Model prediction of a μ differs from the experimental value by 3.2σ.  相似文献   

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The reactionppp f ( + )p s , where the + system is centrally produced, has been studied at 300 GeV/c. The + mass spectrum shows evidence for a 0 decay mode of the (958) andf 1 (1285). The branching ratio (f 1(1285) + +)/(f 1(1285) 0 ) is found to be 5.0±0.7. No evidence is found for a 0(770) decay mode of theE/f 1 (1420) for which an upper limit BR (E/f 1(1420) 0 )<0.08 at=" 95%=" cl=" is=">  相似文献   

7.
We reconsider Muskhelishvili–Omnès (MO) dispersive representations of photon–photon scattering to two pions, motivated by the very high statistics results recently released by the Belle collaboration for charged as well as neutral pion pairs and also by recent progress in the determination of the low-energy π π scattering amplitude. Applicability of this formalism is extended beyond 1 GeV by taking into account inelasticity due to  $K\bar{K}$ . A modified MO representation is derived which has the advantage that all polynomial ambiguities are collected into the subtraction constants and have simple relations to pion polarizabilities. It is obtained by treating differently the exactly known QED Born term and the other components of the left-hand cut. These components are approximated by a sum over resonances. All resonances up to spin two and masses up to ?1.3 GeV are included. The tensor contributions to the left-hand cut are found to be numerically important. We perform fits to the data imposing chiral constraints, in particular, using a model independent sum-rule result on the p 6 chiral coupling c 34. Such theoretical constraints are necessary because the experimental errors are dominantly systematic. Results on further p 6 couplings and pion dipole and quadrupole polarizabilities are then derived from the fit. The relevance of the new data for distinguishing between two possible scenarios of isospin breaking in the f 0(980) region is discussed.  相似文献   

8.
D P Goyal  A V Sodhi 《Pramana》1977,9(1):53-59
Cross-sections for are reported in the centre-of-mass energy interval 1850–2160 MeV. The data come from a deuterium bubble chamber experiment atK beam momenta of 1.45 and 1.65 GeV/c. Taking into account the Fermi motion of the neutron in the deuteron, this momentum range corresponds to the centre-of-mass energy interval of 1850–2160 MeV.  相似文献   

9.
Data for the elastic scattering of 30–80 MeV positive and negative pions by a wide range of nuclei is analysed with an Ericson-Ericson MSU type optical potential. By use of consistent sets of data for π+ and π and of experimental results for total reaction cross sections we obtain for the first time optical potentials that describe well all the data without the need of introducing non-standard charge-dependent effects.  相似文献   

10.
The e + e ? → ω, ρ → π0 e + e ? processes have been investigated in the experiments with Spherical Neutral Detector at the VEPP-2M e + e ? collider. The measurements provide the probability ?(ω → π0 e + e ?) = (0.761 ± 0.053 ± 0.064) × 10?3 of the ω → π0 e + e g- conversion decay and the upper limit ?(ρ → π0 e + e ?) < 1.2 × 10?5 (at 90% CL) for the ρ → π0 e + e ? decay. The transition form factor was measured at three values of the 4-momentum transfer squared.  相似文献   

11.
The cross section for the e + e ? ?? ???0 ?? ??0??0?? process has been measured in the energy range of 1.1?C1.9 GeV. The measurement has been made with the Spherical Neutral Detector at the VEPP-2000 e + e ? collider. The data in the energy range of 1.1?C1.4 GeV are in agreement with the earlier measurements with the SND and CMD-2 detectors. The cross section has also been measured above 1.4 GeV.  相似文献   

12.
In the diffraction dissociation of π? into μ+μ?π? on a Cu nucleus at 50 GeV/c, the cross section \(\sigma _{\mu ^ + \mu ^ - \pi ^ - } \) for the 1+S(ρ0π) wave was measured. The branching ratio of ρ0→μ+μ? could be calculated from the ratio of this and the corresponding cross sections in the diffraction dissociation of π? into π+π?π?. The obtained value \(BR_{\rho ^0 \to \mu ^ + \mu ^ - } = (4.6 \pm 0.2_{stat^ \pm } \pm 0.2_{syst} )10^{ - 5} \) is in good agreement with the branching ratio \(BR_{\rho ^0 \to e^ + e^ - } \) , as expected ifeμ universality holds.  相似文献   

13.
In the experiment withe + e ?-beams performed at the VEPP-4 storage ring with the MD-1 detector we have measuredB μμ, the branching ratio for the decay of Υ(1S) state intoμ + μ ?. We obtainedB μμ=(2.12+0.20+0.10)%. It is shown that the continuum and resonance interference should be taken into account. For the first time the upper limits on the branching ratio for the decaysΥπ + π ?,K + K ?,p \(\bar p\) have been measured: Br(Υπ + π ?)<5·10?4, Br(ΥK + K ?)<5·10?4, Br(Υp \(\bar p\) <9·10?4 (90% CL).  相似文献   

14.
《Physics letters. [Part B]》1986,174(1):115-117
The reaction e+e → ηπ+π has been studied with the Neutral Detector in the CM energy range 1.05–1.40 GeV at VEPP-2M. At the maximum energy the cross section exceeds the prediction of the vector dominance with one ϱ(770). The following upper limits for the electron width times branching ratio into ηπ+π have been obtained for a resonance with a mass of 1.28 GeV and width of 0.08 GeV observed with the Omega-spectrometer at CERN: Λee·Bηππ < 9 eV, and for a ϱ′(1250) with a mass of 1.26 GeV and width of 0.125 GeV: Λee·Bηππ < 14 eV at 90% confidence level.  相似文献   

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The reactionsπ ?p→K 0 0(1385) andπ ? pK + ?(1385) are studied at an incident momentum of 3.95 GeV/c using data from a high statistics bubble chamber experiment corresponding to approximately 90 events/μb. The total and differential cross sections and the density matrix elements of the Σ(1385) are presented. The results are compared with those obtained for the related processesπ pp→K + +(1385) and \(K^ - p \to \pi ^ \mp \sum ^ \pm (1385)\) in this energy range. Evidence is presented for the existence of production mechanisms with exotic exchanges in thet channel.  相似文献   

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Preliminary data on the reactions e + e →φ→γ f 0(980)→γπ0π0 together with data on ππ scattering and the reactions J/ψ→φπ+π and K p→π +π(Λ,Σ) are analyzed. The analysis shows that the mass of the f 0(980) meson is = 950 MeV, and BR(φ→γf 0→γπ0π0)≃ 1× 10−4, indicating that the f 0(980) resonance is of a four-quark nature. Pis’ma Zh. éksp. Teor. Fiz. 67, No. 7, 445–449 (10 April 1998)  相似文献   

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