221 research outputs found

    Compteur Cerenkov differentiel a seuil

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    On nature of the scalar-isoscalar mesons in the uniformizing-variable method based on analyticity and unitarity

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    The experimental data on the processes ππππ,KKˉ,ηη,ηη\pi\pi\to\pi\pi,K\bar{K},\eta\eta,\eta\eta^\prime in the IGJPC=0+0++I^GJ^{PC}=0^+0^{++} channel have been jointly analyzed to study the status and nature of the f0f_0. The method of analysis is based on analyticity and unitarity and uses an uniformization procedure. Some spectroscopic implications from results of the analysis are discussed.Comment: 18 pages, 5 figures, 9 table

    The lightest scalar glueball

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    Recently performed investigations of meson spectra allow us to determine the resonance structure for the waves IJPC=00++IJ^{PC}=00^{++}, 10++10^{++}, 02++02^{++}, 12++12^{++} = IJP=1/20+IJ^P= 1/2 0^+ in the mass region up to 1900 MeV, thus establishing the meson multiplets 13P0qqˉ1^3P_0q\bar q and 23P0qqˉ2^3P_0q\bar q. Experimental data demonstrate that there are five scalar/isoscalar states in this mass region. Four of them are qqˉq\bar q states, that is, members of the 13P0qqˉ1^3P_0q\bar q and 23P0qqˉ2^3P_0q\bar q nonets, while the fifth state is an extra one not accomodated by qqˉq \bar q systematics; it has the properties of the lightest scalar glueball. Analysis of the 00++00^{++}-wave performed within the framework of the dispersion relation technique allows us to reconstruct the mixing of a pure gluonium with neighbouring scalar qqˉq \bar q states belonging to 13P0qqˉ1^3P_0q\bar q and 23P0qqˉ2^3P_0q\bar q nonets: three scalar mesons share the gluonium state between each other -- those are two comparatively narrow resonances f0(1300)f_0(1300) and f0(1500)f_0(1500) and a broad resonance f0(1530250+90)f_0(1530^{+90}_{-250}). The broad state is a descendant of the gluonium, keeping about 40-50% of its component.Comment: 48 pages, LaTeX, 25 PostScript figures, epsfig.sty. Submitted to Russian Journal Uspekhi Fiz. Nauk (Phys-Uspekhi

    Study of the ηπo\eta\pi^o system in the mass range up to 1200 MeV

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    The reaction πpηπon\pi^-p \to \eta\pi^o n has been studied with GAMS-2000 spectrometer in the secondary 38 GeV/c π\pi^--beam of the IHEP U-70 accelerator. Partial wave analysis of the reaction has been performed in the ηπo\eta\pi^o mass range up to 1200 MeV. The a0(980)a_0(980)-meson is seen as a sharp peak in S-wave. The tt-dependence of a0(980)a_0(980) production cross section has been studied. Dominant production of the a0(980)a_0(980) at a small transfer momentum tt confirms the hypothesis of Achasov and Shestakov about significant contribution of the ρ2\rho_2 exchange (IGJPC=1+2I^GJ^{PC}=1^+2^{--}) in the mechanism of a0(980)a_0(980) meson production in tt-channel of the reaction.Comment: 4 pages, 3 figures, talk given at HADRON'9

    The two-pion spectra for the reaction \pi^- p -> \pi^0\pi^0 n at 38 GeV/c pion momentum and combined analysis of the GAMS, Crystal Barrel and BNL data

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    We perform the K-matrix analysis of meson partial waves with IJ^{PC} =00^{++}, 10^{++}, 02^{++}, 12^{++} basing on GAMS data on \pi^-p -> \pi^0\pi^0 n, \eta\eta n, \eta\eta' n together with BNL data on \pi^-p -> K\bar K n and Crystal Barrel data on p\bar p (at rest) -> \pi^0\pi^0\pi^0, \pi^0\eta\eta, \pi^0\pi^0\eta. The positions of the amplitude poles (physical resonances) are determined as well as the positions of the K-matrix poles (bare states) and the values of bare state couplings to two-meson channels. Nonet classification of the determined bare states is discussed.Comment: LaTex, 15 pages and 10 figure

    Process pi p -> pi pi N at high energies and moderate momenta transferred to the nucleon and the determination of parameters of the f_0(980) and f_0(1300)

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    We present the results of simultaneous analysis of the S-wave pi pi-spectra in the reactions pi^- p -> (pi^0 pi^0)_S n at p_{lab}=38 GeV/c (GAMS) and pi^- p -> (pi^+ pi^-)_S n at p_{lab}=18 GeV/c (E852 Collaboration) at moderate momenta transferred to the nucleon, |t| < 1.5 (GeV/c)^2. The t-distributions are described by the reggeized pi- and a_1-exchanges provided by the leading and daughter trajectories, while the M_{pi pi}-spectra are determined by a set of scalar-isoscalar resonances. With M_{pi pi}-distributions averaged over t-intervals, we have found several solutions given by different t-channel exchange mechanisms at |t| ~ (0.5-1.5) (GeV/c)^2, with resonance parameters close to each other. We conclude that despite a poor knowledge of the structure of the t-exchange, the characteristics of resonances such as masses and widths can be reliably determined using the processes under discussion. As to pole positions, we have found (1031 +/- 10) - i(35 +/- 6) MeV for f_0(980) and (1315 +/- 20) - i(150 +/- 30) MeV for f_0(1300).Comment: 17 pages, RevTeX, 10 EPS figures, misprints correcte

    Search for the scalar a0a_0 and f0f_0 mesons in the reactions e+eγπ0π0(η)e^+e^-\to\gamma\pi^0\pi^0(\eta)

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    It is shown that the reactions e+eγπ0π0(η)e^+e^-\to\gamma\pi^0\pi^0(\eta) give a good chance for observing scalar a0a_0 and f0f_0 mesons. In the photon energy region less then 100 MeV the vector meson contributions e+eV0π0V0γπ0π0(η)e^+e^-\to V^0\to\pi^0 V'^0\to\gamma\pi^0\pi^0(\eta) are negligible in comparison with the scalar mesons e+eϕγf0(a0)γπ0π0(η)e^+e^-\to\phi\to\gamma f_0(a_0)\to\gamma\pi^0\pi^0(\eta) for BR(ϕγf0(a0)γπ0π0(η))BR(\phi\to\gamma f_0(a_0)\to\gamma\pi^0\pi^0(\eta)) greater than 5106(105)5\cdot10^{-6}(10^{-5}). Using two-channel treatment of the ππ\pi\pi scattering the predictions for BR(ϕγ(f0+σ)γππ)BR(\phi\to\gamma (f_0+\sigma)\to\gamma\pi\pi) are derived. The four quark model, the model of KKˉK\bar K molecule and thessˉs\bar s model of scalar f0f_0 and a0a_0 mesons are discussed.Comment: 31 pages, 10 ps files of figures, minor numerical changes, Appendix corrected, to be published in Phys.Rev.

    A Study of the \eta \pi^{0} Spectrum and Search for a J^{PC} = 1^{-+} Exotic Meson

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    A partial wave analysis (PWA) of the of the ηπ0\eta \pi ^0 system (where ηγγ\eta \to \gamma \gamma) produced in the charge exchange reaction πpηπ0n\pi ^-p\to \eta \pi ^0n at an incident momentum of 18 GeV/c/c is presented as a function of ηπ0{\eta \pi ^0} invariant mass, mηπ0m_{\eta\pi^0}, and momentum transfer squared, tπηπt_{\pi^{-}\to\eta\pi}, from the incident π\pi^- to the outgoing ηπ0{\eta\pi ^0} system. SS, PP and DD waves were included in the PWA. The a0(980)a_0(980) and a2(1320)a_2(1320) states are clearly observed in the overall ηπ0{\eta\pi ^0} effective mass distribution as well as in the amplitudes associated with SS wave and DD waves respectively after partial wave decomposition. The observed distributions in moments (averages of spherical harmonics) were compared to the results from the PWA and the two are consistent. The distribution in tπηπt_{\pi^{-}\to\eta\pi} for individual DD waves associated with natural and unnatural parity exchange in the tt-channel are consistent with Regge phenomenology. Of particular interest in this study is the PP wave since this leads to an exotic JPC=1+J^{PC}=1^{-+} for the ηπ\eta \pi system. A PP wave is present in the data, however attempts to describe the mass dependence of the amplitude and phase motion with respect to the DD wave as a Breit-Wigner resonance are problematic. This has implications regarding the existence of a reported exotic JPC=1+J^{PC} = 1^{-+} meson decaying into ηπ0\eta \pi^0 with a mass near 1.4 GeV/c2/c^2.Comment: 19 pages, 29 figures, to appear in Phys. Rev.
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