353 research outputs found

    Quasi-fixed point scenario in the modified NMSSM

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    The simplest extension of the MSSM that does not contradict LEP II experimental bound on the lightest Higgs boson mass at tanβ1\tan\beta\sim 1 is the modified Next-to-Minimal Supersymmetric Standard Model (MNSSM). We investigate the renormalization of Yukawa couplings and soft SUSY breaking terms in this model. The possibility of bb-quark and τ\tau-lepton Yukawa coupling unification at the Grand Unification scale MXM_X is studied. The particle spectrum is analysed in the vicinity of the quasi-fixed point where the solutions of renormalization group equations are concentrated at the electroweak scale.Comment: 19 pages, 3 figures, LaTeX2

    Infrared quasi-fixed solutions in the NMSSM

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    The considerable part of the parameter space in the MSSM corresponding to the infrared quasi fixed point scenario is almost excluded by LEP II bounds on the lightest Higgs boson mass. In the NMSSM the mass of the lightest Higgs boson reaches its maximum value in the strong Yukawa coupling limit when Yukawa couplings are essentially larger than gauge ones at the Grand Unification scale. In this limit the solutions of the renormalisation group equations are attracted to the infrared and Hill type effective fixed lines or surfaces in the Yukawa coupling parameter space. They are concentrated in the vicinity of quasi fixed points for Yi(0)Y_i(0)\to\infty. However the solutions are attracted to such points rather weakly. For this reason when all Yi(0)1Y_i(0)\sim 1 the solutions of the renormalisation group equations are gathered near a line in the Hill type effective surface. In the paper the approximate solutions for the NMSSM Yukawa couplings are given. The possibility of bb--quark and τ\tau--lepton Yukawa coupling unification at the scale MXM_{X} is also discussed.Comment: 32 pages, 8 figures included, LaTeX 2

    Resonance-like coherent production of a pion pair in the reaction pdpdππpd \rightarrow pd\pi\pi in the GeV region

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    The reaction p+dp+d+Xp + d \rightarrow p + d + X was studied at 0.8-2.0 GeV proton beam energies with the ANKE magnetic spectrometer at the COSY synchrotron storage ring. The proton-deuteron pairs emerging with high momenta, 0.6-1.8 GeV/cc, were detected at small angles with respect to the proton beam. Distribution over the reaction missing mass MxM_x reveals a local enhancement near the threshold of the pion pair production specific for the so-called ABC effect. The enhancement has a structure of a narrow bump placed above a smooth continuum. The invariant mass of the dππd\pi\pi system in this enhancement region exhibits a resonance-like peak at Mdππ2.36M_{d\pi\pi} \approx 2.36 GeV/c2c^2 with the width Γ0.10\Gamma \approx 0.10 GeV/c2c^2. A possible interpretation of these features is discussed.Comment: 14 pages, 16 figures, submitted to Eur. Phys. J. A. v2: Added references [42,43] in section IV.A. v3: revised version according to referee remarks v4: revised version according to referee remark

    gDsDK(892)g_{D^{\ast}_{s}D K^{\ast}(892)} and gBsBK(892)g_{B^{\ast}_{s}B K^{\ast}(892)} coupling constants in QCD sum rules

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    The coupling constants gDsDK(892)g_{D^{\ast}_{s}D K^{\ast}(892)} and gBsBK(892)g_{B^{\ast}_{s}B K^{\ast}(892)} are calculated in the framework of three-point QCD sum rules. The correlation functions responsible for these coupling constants are evaluated considering contributions of both D(B)D(B) and K(892)K^*(892) mesons as off-shell states, but in the absence of radiative corrections. The results, gDsDK(892)=(4.31±1.42)GeV1g_{D^{\ast}_{s}D K^{\ast}(892)}=(4.31\pm1.42) GeV^{-1} and gBsBK(892)=(3.24±1.08)GeV1g_{B^{\ast}_{s}B K^{\ast}(892)}=(3.24\pm1.08) GeV^{-1} are obtained for the considered strong coupling constants.Comment: 13 Pages and 11 Figure

    The heavy baryons in the nonperturbative string approach

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    We present some piloting calculations of the short-range correlation coefficients for the light and heavy baryons and masses of the doubly heavy baryons ΞQQ\Xi_{QQ'} and ΩQQ\Omega_{QQ'} (Q,Q=c,bQ,Q'=c,b) in the framework of the simple approximation within the nonperturbative QCD approach.Comment: 21 pages; to appear in Phys. Atom. Nuc

    First measurements of spin correlations in the np -> d pi^0 reaction

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    The transverse spin correlations Axx and Ayy in the np-> d pi^0 reaction have been measured for the first time in quasi-free kinematics at the COSY-ANKE facility using a polarised deuteron beam incident on a polarised hydrogen cell target. The results obtained for neutron energies close to 353 MeV and 600 MeV are in good agreement with the partial wave analysis of data on the isospin-related pp-> d pi^+ reaction, though the present results cover also the small-angle region, which was largely absent from these data

    Higgs bosons in the simplest SUSY models

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    Nowadays in the MSSM the moderate values of tanβ\tan\beta are almost excluded by LEP II lower bound on the lightest Higgs boson mass. In the Next-to-Minimal Supersymmetric Standard Model the theoretical upper bound on it increases and reaches maximal value in the strong Yukawa coupling limit when all solutions of renormalization group equations are concentrated near the quasi-fixed point. For calculation of Higgs boson spectrum the perturbation theory method can be applied. We investigate the particle spectrum in the framework of the modified NMSSM which leads to the self-consistent solution in the strong Yukawa coupling limit. This model allows one to get mh125m_h\sim 125 GeV at values of tanβ1.9\tan\beta\ge 1.9. In the investigated model the lightest Higgs boson mass does not exceed 130.5±3.5130.5\pm 3.5 GeV. The upper bound on the lightest CP-even Higgs boson mass in more complicated supersymmetric models is also discussed.Comment: 27 pages, 5 figures included, LaTeX 2e. Plenary talk at the Conference of RAS Nuclear Physics Department 2000 in ITEP, Moscow, Russia; to appear in Phys. Atom. Nuc

    Measurement of the analyzing powers in pd elastic and pn quasi-elastic scattering at small angles

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    The analyzing powers in proton-deuteron elastic and proton-neutron quasi-elastic scattering have been measured at small angles using a polarized proton beam at the COSY storage ring incident on an unpolarized deuterium target. The data were taken at 796MeV and five higher energies from 1600MeV to 2400MeV. The analyzing power in pd elastic scattering was studied by detecting the low energy recoil deuteron in telescopes placed symmetrically in the COSY plane to the left and right of the beam whereas for pn quasi-elastic scattering a low energy proton was registered in one of the telescopes in coincidence with a fast scattered proton measured in the ANKE magnetic spectrometer. Though the experiment explores new domains, the results are consistent with the limited published information.Comment: 10 pages with 8 figure

    Coherent pion production in proton-deuteron collisions

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    Values of the proton analysing power in the pd3Heπ0/3Hπ+pd\to{}^{3}\textrm{He}\,\pi^0/^{3}\textrm{H}\,\pi^+ reactions at 350-360~MeV per nucleon were obtained by using a polarised proton beam incident on a deuterium cluster-jet target and with a polarised deuteron beam incident on a target cell filled with polarised hydrogen. These results have a much larger angular coverage than existing data. First measurements are also presented of the deuteron vector analysing power and the deuteron-proton spin correlations. Data were also obtained on the deuteron-proton spin correlation and proton analysing power at small angles at 600~MeV per nucleon, though the angular coverage at this energy was much more restricted even when using a deuteron beam. By combining the extrapolated values of the spin correlations to the forward or backward directions with published measurements of the deuteron tensor analysing powers, the relative phases between the two non-vanishing amplitudes were evaluated.Comment: 5 pages, 5 figure

    Measurement of the analysing power in proton-proton elastic scattering at small angles

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    The proton analysing power in pp\vec{p}p elastic scattering has been measured at small angles at COSY-ANKE at 796 MeV and five other beam energies between 1.6 and 2.4 GeV using a polarised proton beam. The asymmetries obtained by detecting the fast proton in the ANKE forward detector or the slow recoil proton in a silicon tracking telescope are completely consistent. Although the analysing power results agree well with the many published data at 796 MeV, and also with the most recent partial wave solution at this energy, the ANKE data at the higher energies lie well above the predictions of this solution at small angles. An updated phase shift analysis that uses the ANKE results together with the World data leads to a much better description of these new measurements.Comment: 5 pages, 3 figure
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