42 research outputs found

    Ground-state triply and doubly heavy baryons in a relativistic three-quark model

    Full text link
    Mass spectra of the ground-state baryons consisting of three or two heavy (b or c) and one light (u,d,s) quarks are calculated in the framework of the relativistic quark model and the hyperspherical expansion. The predictions of masses of the triply and doubly heavy baryons are obtained by employing the perturbation theory for the spin-independent and spin-dependent parts of the three-quark Hamiltonian.Comment: 10 pages, 2 figures, LaTe

    ΠœΠΎΠ·Π°ΠΈΡ‡Π½Π°Ρ аутологичная остСохондропластика Π² Π»Π΅Ρ‡Π΅Π½ΠΈΠΈ локального асСптичСского Π½Π΅ΠΊΡ€ΠΎΠ·Π° Π±Π»ΠΎΠΊΠ° Ρ‚Π°Ρ€Π°Π½Π½ΠΎΠΉ кости

    Get PDF
    The authors presented the brief incidence analysis of talus osteochondral defect (local joint surface osteonecrosis of the anklebone), its etiology, pathogenesis, symptoms, modern diagnostic algorithm and described proposed surgical procedure. The operation consists of ankle joint arthrotomy, osteonecrotic tissue resection, harvesting of cylindrical mosaic osteochondral graft from low weightbared region of femoral knee joint surface and its implantation into resection cave of the anklebone. The indications to supramalleolar osteotomy for concomitant ankle frontal deformities are grounded. Rigid osteosynthesis and early movements in ankle joint are recommended. Eighteen patients with age from 20 to 58 years old were operated: 8 men and 10 women. In 13 cases (72.3%) the lesion was found in medial edge of talus trochlea, and 5 (27.7%) were lateral lesions. Treatment results of 18 patients evaluated according AOFAS score (H. Kitaoka) improved after operation from (38.2+3.3), to (88.9+3.6) when assessed one year after surgery. Two clinical case reports are presented.ΠŸΡ€ΠΎΠ²Π΅Π΄Π΅Π½Ρ‹ ΠΊΡ€Π°Ρ‚ΠΊΠΈΠΉ Π°Π½Π°Π»ΠΈΠ· частоты локального остСонСкроза Π±Π»ΠΎΠΊΠ° Ρ‚Π°Ρ€Π°Π½Π½ΠΎΠΉ кости, Π΅Π³ΠΎ этиология, ΠΏΠ°Ρ‚ΠΎΠ³Π΅Π½Π΅Π·, симптоматика, соврСмСнныС ΠΏΡ€ΠΈΠ½Ρ†ΠΈΠΏΡ‹ диагностики. ΠŸΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½Π° ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΈΠΊΠ° хирургичСского лСчСния, Π²ΠΊΠ»ΡŽΡ‡Π°ΡŽΡ‰Π°Ρ Π°Ρ€Ρ‚Ρ€ΠΎΡ‚ΠΎΠΌΠΈΡŽ голСностопного сустава, Ρ€Π΅Π·Π΅ΠΊΡ†ΠΈΡŽ патологичСского ΠΎΡ‡Π°Π³Π°, взятиС ΠΈΠ· Π½Π΅Π½Π°Π³Ρ€ΡƒΠΆΠ°Π΅ΠΌΠΎΠΉ Π·ΠΎΠ½Ρ‹ Π±Π΅Π΄Ρ€Π° ΠΌΠΎΠ·Π°ΠΈΡ‡Π½ΠΎΠ³ΠΎ цилиндричСского костнохрящСвого аутотрансплантата с ΠΏΠΎΡΠ»Π΅Π΄ΡƒΡŽΡ‰Π΅ΠΉ Π΅Π³ΠΎ ΠΈΠΌΠΏΠ»Π°Π½Ρ‚Π°Ρ†ΠΈΠ΅ΠΉ Π² Π·ΠΎΠ½Ρƒ Π΄Π΅Ρ„Π΅ΠΊΡ‚Π° Ρ‚Π°Ρ€Π°Π½Π½ΠΎΠΉ кости. ΠŸΡ€ΠΈ Π½Π°Π»ΠΈΡ‡ΠΈΠΈ Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… Π½Π°Ρ€ΡƒΡˆΠ΅Π½ΠΈΠΉ анатомичСских осСй Π² голСностопном суставС ΠΎΠ΄Π½ΠΎΠΌΠΎΠΌΠ΅Π½Ρ‚Π½ΠΎ ΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈ ΠΊΠΎΡ€Ρ€ΠΈΠ³ΠΈΡ€ΡƒΡŽΡ‰ΡƒΡŽ ΠΎΡΡ‚Π΅ΠΎΡ‚ΠΎΠΌΠΈΡŽ Π±ΠΎΠ»ΡŒΡˆΠ΅Π±Π΅Ρ€Ρ†ΠΎΠ²ΠΎΠΉ кости с остСосинтСзом мСталличСской пластиной. Π‘ использованиСм описанной хирургичСской Ρ‚Π΅Ρ…Π½ΠΈΠΊΠΈ ΠΏΡ€ΠΎΠΎΠΏΠ΅Ρ€ΠΈΡ€ΠΎΠ²Π°Π½Ρ‹ 18 ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ² Π² возрастС ΠΎΡ‚ 20 Π΄ΠΎ 58 Π»Π΅Ρ‚: 8 ΠΌΡƒΠΆΠΈΡ‡ΠΈΠ½ ΠΈ 10 ΠΆΠ΅Π½Ρ‰ΠΈΠ½. Π’ 13 (72,3%) случаях ΠΎΡ‚ΠΌΠ΅Ρ‡Π°Π»ΠΎΡΡŒ ΠΏΠΎΡ€Π°ΠΆΠ΅Π½ΠΈΠ΅ мСдиального ΠΎΡ‚Π΄Π΅Π»Π° Π±Π»ΠΎΠΊΠ° Ρ‚Π°Ρ€Π°Π½Π½ΠΎΠΉ кости, Π² 5 (27,7%) - Π½Π°Ρ€ΡƒΠΆΠ½ΠΎΠ³ΠΎ ΠΎΡ‚Π΄Π΅Π»Π°. Π‘Ρ€Π΅Π΄Π½ΠΈΠΉ Π±Π°Π»Π» ΠΈΠ½Ρ‚Π΅Π³Ρ€Π°Π»ΡŒΠ½ΠΎΠΉ ΠΎΡ†Π΅Π½ΠΊΠΈ состояния голСностопного сустава ΠΏΠΎ шкалС AOFAS (H. Kitaoka) Ρƒ всСх ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ² Π΄ΠΎ ΠΎΠΏΠ΅Ρ€Π°Ρ†ΠΈΠΈ составлял 38,2Β±3,3, Ρ‡Π΅Ρ€Π΅Π· Π³ΠΎΠ΄ послС описанной ΠΎΠΏΠ΅Ρ€Π°Ρ†ΠΈΠΈ - 88,9Β±3,6. ΠŸΡ€Π΅Π΄ΡΡ‚Π°Π²Π»Π΅Π½Ρ‹ Π΄Π²Π° клиничСских наблюдСния. ΠŸΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ Π°ΡƒΡ‚ΠΎΠ»ΠΎΠ³ΠΈΡ‡Π½ΠΎΠΉ ΠΌΠΎΠ·Π°ΠΈΡ‡Π½ΠΎΠΉ остСохондропластики ΠΏΡ€ΠΈ хирургичСском Π»Π΅Ρ‡Π΅Π½ΠΈΠΈ Π΄Π΅Ρ„Π΅ΠΊΡ‚ΠΎΠ² Ρ‚Π°Ρ€Π°Π½Π½ΠΎΠΉ кости позволяСт ΠΏΠΎΠ»ΡƒΡ‡ΠΈΡ‚ΡŒ ΡƒΠ΄ΠΎΠ²Π»Π΅Ρ‚Π²ΠΎΡ€ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Π΅ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ лСчСния ΠΈ Π²ΠΎΡΡΡ‚Π°Π½ΠΎΠ²ΠΈΡ‚ΡŒ анатомичСскоС строСниС ΠΈ Π±ΠΈΠΎΠΌΠ΅Ρ…Π°Π½ΠΈΠΊΡƒ голСностопного сустава

    Confinement and Chiral Symmetry Breaking via Domain-Like Structures in the QCD Vacuum

    Get PDF
    A qualitative mechanism for the emergence of domain structured background gluon fields due to singularities in gauge field configurations is considered, and a model displaying a type of mean field approximation to the QCD partition function based on this mechanism is formulated. Estimation of the vacuum parameters (gluon condensate, topological susceptibility, string constant and quark condensate) indicates that domain-like structures lead to an area law for the Wilson loop, nonzero topological susceptibility and spontaneous breakdown of chiral symmetry. Gluon and ghost propagators in the presence of domains are calculated explicitly and their analytical properties are discussed. The Fourier transforms of the propagators are entire functions and thus describe confined dynamical fields.Comment: RevTeX, 48 pages (32 pages + Appendices A-E), new references added [1,2,4,5] and minor formulae corrected for typographical error

    Properties of heavy quarkonia and B_c mesons in the relativistic quark model

    Get PDF
    The mass spectra and electromagnetic decay rates of charmonium, bottomonium and B_c mesons are comprehensively investigated in the relativistic quark model. The presence of only heavy quarks allows the expansion in powers of their velocities. All relativistic corrections of order v^2/c^2, including retardation effects and one-loop radiative corrections, are systematically taken into account in the computations of the mass spectra. The obtained wave functions are used for the calculation of radiative magnetic dipole (M1) and electric dipole (E1) transitions. It is found that relativistic effects play a substantial role. Their account and the proper choice of the Lorentz structure of the quark-antiquark interaction in a meson is crucial for bringing theoretical predictions in accord with experimental data. A detailed comparison of the calculated decay rates and branching fractions with available experimental data for radiative decays of charmonium and bottomonium is presented. The possibilities to observe the currently missing spin-singlet S and P states as well as D states in bottomonium are discussed. The results for B_c masses and decays are compared with other quark model predictions.Comment: 31 pages, 2 figures, minor correction

    The BES f_0(1810): a new glueball candidate

    Get PDF
    We analyze the f_0(1810) state recently observed by the BES collaboration via radiative J/\psi decay to a resonant \phi\omega spectrum and confront it with DM2 data and glueball theory. The DM2 group only measured \omega\omega decays and reported a pseudoscalar but no scalar resonance in this mass region. A rescattering mechanism from the open flavored KKbar decay channel is considered to explain why the resonance is only seen in the flavor asymmetric \omega\phi branch along with a discussion of positive C parity charmonia decays to strengthen the case for preferred open flavor glueball decays. We also calculate the total glueball decay width to be roughly 100 MeV, in agreement with the narrow, newly found f_0, and smaller than the expected estimate of 200-400 MeV. We conclude that this discovered scalar hadron is a solid glueball candidate and deserves further experimental investigation, especially in the K-Kbar channel. Finally we comment on other, but less likely, possible assignments for this state.Comment: 11 pages, 4 figures. Major substantive additions, including an ab-initio, QCD-based computation of the glueball inclusive decay width, evaluation of final state effects, and enhanced discussion of several alternative possibilities. Our conclusions are unchanged: the BES f_0(1810) is a promising glueball candidat

    Mass spectra of doubly heavy Omega_QQ' baryons

    Full text link
    We evaluate the masses of baryons composed of two heavy quarks and a strange quark with account for spin-dependent splittings in the framework of potential model with the KKO potential motivated by QCD with a three-loop beta-function for the effective charge consistent with both the perturbative limit at short distances and linear confinement term at long distances between the quarks. The factorization of dynamics is supposed and explored in the nonrelativistic Schroedinger equation for the motion in the system of two heavy quarks constituting the doubly heavy diquark and the strange quark interaction with the diquark. The limits of approach, its justification and uncertainties are discussed. Excited quasistable states are classified by the quantum numbers of heavy diquark composed by the heavy quarks of the same flavor.Comment: 14 pages, revtex4-file, 3 eps-figures, 5 tables, typos correcte

    Measurement of RudsR_{\text{uds}} and RR between 3.12 and 3.72 GeV at the KEDR detector

    Get PDF
    Using the KEDR detector at the VEPP-4M e+eβˆ’e^+e^- collider, we have measured the values of RudsR_{\text{uds}} and RR at seven points of the center-of-mass energy between 3.12 and 3.72 GeV. The total achieved accuracy is about or better than 3.3%3.3\% at most of energy points with a systematic uncertainty of about 2.1%2.1\%. At the moment it is the most accurate measurement of R(s)R(s) in this energy range

    New precise determination of the \tau lepton mass at KEDR detector

    Full text link
    The status of the experiment on the precise Ο„\tau lepton mass measurement running at the VEPP-4M collider with the KEDR detector is reported. The mass value is evaluated from the Ο„+Ο„βˆ’\tau^+\tau^- cross section behaviour around the production threshold. The preliminary result based on 6.7 pbβˆ’1^{-1} of data is mΟ„=1776.80βˆ’0.23+0.25Β±0.15m_{\tau}=1776.80^{+0.25}_{-0.23} \pm 0.15 MeV. Using 0.8 pbβˆ’1^{-1} of data collected at the Οˆβ€²\psi' peak the preliminary result is also obtained: Ξ“eeBττ(Οˆβ€²)=7.2Β±2.1\Gamma_{ee}B_{\tau\tau}(\psi') = 7.2 \pm 2.1 eV.Comment: 6 pages, 8 figures; The 9th International Workshop on Tau-Lepton Physics, Tau0

    Measurement of \Gamma_{ee}(J/\psi)*Br(J/\psi->e^+e^-) and \Gamma_{ee}(J/\psi)*Br(J/\psi->\mu^+\mu^-)

    Get PDF
    The products of the electron width of the J/\psi meson and the branching fraction of its decays to the lepton pairs were measured using data from the KEDR experiment at the VEPP-4M electron-positron collider. The results are \Gamma_{ee}(J/\psi)*Br(J/\psi->e^+e^-)=(0.3323\pm0.0064\pm0.0048) keV, \Gamma_{ee}(J/\psi)*Br(J/\psi->\mu^+\mu^-)=(0.3318\pm0.0052\pm0.0063) keV. Their combinations \Gamma_{ee}\times(\Gamma_{ee}+\Gamma_{\mu\mu})/\Gamma=(0.6641\pm0.0082\pm0.0100) keV, \Gamma_{ee}/\Gamma_{\mu\mu}=1.002\pm0.021\pm0.013 can be used to improve theaccuracy of the leptonic and full widths and test leptonic universality. Assuming e\mu universality and using the world average value of the lepton branching fraction, we also determine the leptonic \Gamma_{ll}=5.59\pm0.12 keV and total \Gamma=94.1\pm2.7 keV widths of the J/\psi meson.Comment: 7 pages, 6 figure

    Search for narrow resonances in e+ e- annihilation between 1.85 and 3.1 GeV with the KEDR Detector

    Full text link
    We report results of a search for narrow resonances in e+ e- annihilation at center-of-mass energies between 1.85 and 3.1 GeV performed with the KEDR detector at the VEPP-4M e+ e- collider. The upper limit on the leptonic width of a narrow resonance Gamma(R -> ee) Br(R -> hadr) < 120 eV has been obtained (at 90 % C.L.)
    corecore