42 research outputs found
Ground-state triply and doubly heavy baryons in a relativistic three-quark model
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
ΠΠΎΠ·Π°ΠΈΡΠ½Π°Ρ Π°ΡΡΠΎΠ»ΠΎΠ³ΠΈΡΠ½Π°Ρ ΠΎΡΡΠ΅ΠΎΡ ΠΎΠ½Π΄ΡΠΎΠΏΠ»Π°ΡΡΠΈΠΊΠ° Π² Π»Π΅ΡΠ΅Π½ΠΈΠΈ Π»ΠΎΠΊΠ°Π»ΡΠ½ΠΎΠ³ΠΎ Π°ΡΠ΅ΠΏΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π½Π΅ΠΊΡΠΎΠ·Π° Π±Π»ΠΎΠΊΠ° ΡΠ°ΡΠ°Π½Π½ΠΎΠΉ ΠΊΠΎΡΡΠΈ
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.ΠΡΠΎΠ²Π΅Π΄Π΅Π½Ρ ΠΊΡΠ°ΡΠΊΠΈΠΉ Π°Π½Π°Π»ΠΈΠ· ΡΠ°ΡΡΠΎΡΡ Π»ΠΎΠΊΠ°Π»ΡΠ½ΠΎΠ³ΠΎ ΠΎΡΡΠ΅ΠΎΠ½Π΅ΠΊΡΠΎΠ·Π° Π±Π»ΠΎΠΊΠ° ΡΠ°ΡΠ°Π½Π½ΠΎΠΉ ΠΊΠΎΡΡΠΈ, Π΅Π³ΠΎ ΡΡΠΈΠΎΠ»ΠΎΠ³ΠΈΡ, ΠΏΠ°ΡΠΎΠ³Π΅Π½Π΅Π·, ΡΠΈΠΌΠΏΡΠΎΠΌΠ°ΡΠΈΠΊΠ°, ΡΠΎΠ²ΡΠ΅ΠΌΠ΅Π½Π½ΡΠ΅ ΠΏΡΠΈΠ½ΡΠΈΠΏΡ Π΄ΠΈΠ°Π³Π½ΠΎΡΡΠΈΠΊΠΈ. ΠΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½Π° ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠ° Ρ
ΠΈΡΡΡΠ³ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π»Π΅ΡΠ΅Π½ΠΈΡ, Π²ΠΊΠ»ΡΡΠ°ΡΡΠ°Ρ Π°ΡΡΡΠΎΡΠΎΠΌΠΈΡ Π³ΠΎΠ»Π΅Π½ΠΎΡΡΠΎΠΏΠ½ΠΎΠ³ΠΎ ΡΡΡΡΠ°Π²Π°, ΡΠ΅Π·Π΅ΠΊΡΠΈΡ ΠΏΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΎΡΠ°Π³Π°, Π²Π·ΡΡΠΈΠ΅ ΠΈΠ· Π½Π΅Π½Π°Π³ΡΡΠΆΠ°Π΅ΠΌΠΎΠΉ Π·ΠΎΠ½Ρ Π±Π΅Π΄ΡΠ° ΠΌΠΎΠ·Π°ΠΈΡΠ½ΠΎΠ³ΠΎ ΡΠΈΠ»ΠΈΠ½Π΄ΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΊΠΎΡΡΠ½ΠΎΡ
ΡΡΡΠ΅Π²ΠΎΠ³ΠΎ Π°ΡΡΠΎΡΡΠ°Π½ΡΠΏΠ»Π°Π½ΡΠ°ΡΠ° Ρ ΠΏΠΎΡΠ»Π΅Π΄ΡΡΡΠ΅ΠΉ Π΅Π³ΠΎ ΠΈΠΌΠΏΠ»Π°Π½ΡΠ°ΡΠΈΠ΅ΠΉ Π² Π·ΠΎΠ½Ρ Π΄Π΅ΡΠ΅ΠΊΡΠ° ΡΠ°ΡΠ°Π½Π½ΠΎΠΉ ΠΊΠΎΡΡΠΈ. ΠΡΠΈ Π½Π°Π»ΠΈΡΠΈΠΈ Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΡΡ
Π½Π°ΡΡΡΠ΅Π½ΠΈΠΉ Π°Π½Π°ΡΠΎΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΎΡΠ΅ΠΉ Π² Π³ΠΎΠ»Π΅Π½ΠΎΡΡΠΎΠΏΠ½ΠΎΠΌ ΡΡΡΡΠ°Π²Π΅ ΠΎΠ΄Π½ΠΎΠΌΠΎΠΌΠ΅Π½ΡΠ½ΠΎ ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈ ΠΊΠΎΡΡΠΈΠ³ΠΈΡΡΡΡΡΡ ΠΎΡΡΠ΅ΠΎΡΠΎΠΌΠΈΡ Π±ΠΎΠ»ΡΡΠ΅Π±Π΅ΡΡΠΎΠ²ΠΎΠΉ ΠΊΠΎΡΡΠΈ Ρ ΠΎΡΡΠ΅ΠΎΡΠΈΠ½ΡΠ΅Π·ΠΎΠΌ ΠΌΠ΅ΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΏΠ»Π°ΡΡΠΈΠ½ΠΎΠΉ. Π‘ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΎΠΏΠΈΡΠ°Π½Π½ΠΎΠΉ Ρ
ΠΈΡΡΡΠ³ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠ΅Ρ
Π½ΠΈΠΊΠΈ ΠΏΡΠΎΠΎΠΏΠ΅ΡΠΈΡΠΎΠ²Π°Π½Ρ 18 ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Π² Π²ΠΎΠ·ΡΠ°ΡΡΠ΅ ΠΎΡ 20 Π΄ΠΎ 58 Π»Π΅Ρ: 8 ΠΌΡΠΆΠΈΡΠΈΠ½ ΠΈ 10 ΠΆΠ΅Π½ΡΠΈΠ½. Π 13 (72,3%) ΡΠ»ΡΡΠ°ΡΡ
ΠΎΡΠΌΠ΅ΡΠ°Π»ΠΎΡΡ ΠΏΠΎΡΠ°ΠΆΠ΅Π½ΠΈΠ΅ ΠΌΠ΅Π΄ΠΈΠ°Π»ΡΠ½ΠΎΠ³ΠΎ ΠΎΡΠ΄Π΅Π»Π° Π±Π»ΠΎΠΊΠ° ΡΠ°ΡΠ°Π½Π½ΠΎΠΉ ΠΊΠΎΡΡΠΈ, Π² 5 (27,7%) - Π½Π°ΡΡΠΆΠ½ΠΎΠ³ΠΎ ΠΎΡΠ΄Π΅Π»Π°. Π‘ΡΠ΅Π΄Π½ΠΈΠΉ Π±Π°Π»Π» ΠΈΠ½ΡΠ΅Π³ΡΠ°Π»ΡΠ½ΠΎΠΉ ΠΎΡΠ΅Π½ΠΊΠΈ ΡΠΎΡΡΠΎΡΠ½ΠΈΡ Π³ΠΎΠ»Π΅Π½ΠΎΡΡΠΎΠΏΠ½ΠΎΠ³ΠΎ ΡΡΡΡΠ°Π²Π° ΠΏΠΎ ΡΠΊΠ°Π»Π΅ AOFAS (H. Kitaoka) Ρ Π²ΡΠ΅Ρ
ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Π΄ΠΎ ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΈ ΡΠΎΡΡΠ°Π²Π»ΡΠ» 38,2Β±3,3, ΡΠ΅ΡΠ΅Π· Π³ΠΎΠ΄ ΠΏΠΎΡΠ»Π΅ ΠΎΠΏΠΈΡΠ°Π½Π½ΠΎΠΉ ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΈ - 88,9Β±3,6. ΠΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Ρ Π΄Π²Π° ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΈΡ
Π½Π°Π±Π»ΡΠ΄Π΅Π½ΠΈΡ. ΠΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ Π°ΡΡΠΎΠ»ΠΎΠ³ΠΈΡΠ½ΠΎΠΉ ΠΌΠΎΠ·Π°ΠΈΡΠ½ΠΎΠΉ ΠΎΡΡΠ΅ΠΎΡ
ΠΎΠ½Π΄ΡΠΎΠΏΠ»Π°ΡΡΠΈΠΊΠΈ ΠΏΡΠΈ Ρ
ΠΈΡΡΡΠ³ΠΈΡΠ΅ΡΠΊΠΎΠΌ Π»Π΅ΡΠ΅Π½ΠΈΠΈ Π΄Π΅ΡΠ΅ΠΊΡΠΎΠ² ΡΠ°ΡΠ°Π½Π½ΠΎΠΉ ΠΊΠΎΡΡΠΈ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΠ΅Ρ ΠΏΠΎΠ»ΡΡΠΈΡΡ ΡΠ΄ΠΎΠ²Π»Π΅ΡΠ²ΠΎΡΠΈΡΠ΅Π»ΡΠ½ΡΠ΅ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ Π»Π΅ΡΠ΅Π½ΠΈΡ ΠΈ Π²ΠΎΡΡΡΠ°Π½ΠΎΠ²ΠΈΡΡ Π°Π½Π°ΡΠΎΠΌΠΈΡΠ΅ΡΠΊΠΎΠ΅ ΡΡΡΠΎΠ΅Π½ΠΈΠ΅ ΠΈ Π±ΠΈΠΎΠΌΠ΅Ρ
Π°Π½ΠΈΠΊΡ Π³ΠΎΠ»Π΅Π½ΠΎΡΡΠΎΠΏΠ½ΠΎΠ³ΠΎ ΡΡΡΡΠ°Π²Π°
Confinement and Chiral Symmetry Breaking via Domain-Like Structures in the QCD Vacuum
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
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
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
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 and between 3.12 and 3.72 GeV at the KEDR detector
Using the KEDR detector at the VEPP-4M collider, we have measured
the values of and 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 at most of energy points with a systematic uncertainty of
about . At the moment it is the most accurate measurement of in
this energy range
New precise determination of the \tau lepton mass at KEDR detector
The status of the experiment on the precise lepton mass measurement
running at the VEPP-4M collider with the KEDR detector is reported. The mass
value is evaluated from the cross section behaviour around the
production threshold. The preliminary result based on 6.7 pb of data is
MeV. Using 0.8 pb of data
collected at the peak the preliminary result is also obtained:
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^-)
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
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.)