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Skachkov, N.B.
Joint Inst. for Nuclear Research, Dubna (USSR). Lab. of Theoretical Physics1974
Joint Inst. for Nuclear Research, Dubna (USSR). Lab. of Theoretical Physics1974
AbstractAbstract
No abstract available
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Source
1974; 9 p; 9 refs.
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Skachkov, N.B.
Joint Inst. for Nuclear Research, Dubna (USSR). Lab. of Theoretical Physics1973
Joint Inst. for Nuclear Research, Dubna (USSR). Lab. of Theoretical Physics1973
AbstractAbstract
No abstract available
Primary Subject
Source
1973; 26 p; 17 refs.; 3 figs.
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AbstractAbstract
[en] A theoretical model that predicts the existence of a new vector meson with the mass of M=1100 MeV in the spectrum of the vector mesons was proposed earlier. The main feature of the model is the use of a new type of the potential that binds two quarks inside a meson. The rho-meson excited state spectra and I/PSI particle mass spectrum are considered. All three particles appearing in the mass spectrum of the model exist in nature, provided that the quantum numbers of new vector meson coincide with the quantum numbers of the rho-meson as the model predicts. The model requires more than one (charmed) heavy quark in order to describe the I/PSI particle spectrum
Primary Subject
Source
Joint Inst. for Nuclear Research, Dubna (USSR); p. C114-C116; 1977; 18. international conference on high energy physics; Tbilisi, USSR; 15 - 21 Jul 1976; 10 refs.; 1 fig.
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Skachkov, N.B.
Joint Inst. for Nuclear Research, Dubna (Russian Federation). Lab. of Theoretical Physics1995
Joint Inst. for Nuclear Research, Dubna (Russian Federation). Lab. of Theoretical Physics1995
AbstractAbstract
[en] The next-to-leading order QCD analysis of the fragmentation functions obtained from new DELPHI data and the data of other collaborations on the inclusive hadron production e+e-→h+X is performed. The data included into analysis belong to the interval of high momentum transfer: 196 GeV2≤Q2≤8312 GeV2 and the value of z(z=Eh/Ebeam)>0.18. The number of flavours was taken to be Nf=5. The fit to these data has given the results: Λ(5)/MS=151-73+101 MeV or αs(Mz2)=0.111-0.009+0.009. 22 refs
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1995; 11 p
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Report
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Skachkov, N.B.
Joint Inst. for Nuclear Research, Dubna (USSR). Lab. of Theoretical Physics1974
Joint Inst. for Nuclear Research, Dubna (USSR). Lab. of Theoretical Physics1974
AbstractAbstract
No abstract available
Primary Subject
Source
1974; 7 p; 7 refs.; submitted to the journal Physics Letters.
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AbstractAbstract
[en] The relativistic quasi-potential method of description of states in the quantum field theory is used for studying the spectrum of mesons considered as a bound state of a quark and an artiquark with 1/2 spins. The formulation of the Kadyshevskij quasi-potential equation in the relativistic configuration representation serves as a starting point. It is shown that the extention of the relativistic configuration representation to small distances permits to introduce into consideration a new class of cutoff potentials of quarks by a theoretic group method. The appearance of the quark cutoff potentials in the proposed approach is the consequence of the choice of a new class of unitary irreducible representations of the Lorentz group - the additional series - for the formulation of the quark dynamics. For the explanation of the I/PSI/-particle spectrum in the quark cutoff model considered with the potential of the relativistic Coulomb potential type it is necessary to introduce more than one heavy quark with different masses
Original Title
Relyativistskoe opisanie sistemy dvukh fermionov na malykh rasstoyaniyakh, novyj vektornyj mezon s massoj M=1110 MeV i spektr I/PSI-chastits
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Source
Joint Inst. for Nuclear Research, Dubna (USSR); p. 526-548; 1977; p. 526-548; 10. International school on high energy physics for young scientists; Baku, USSR; 25 Sep - 5 Oct 1976; 23 refs.
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ANGULAR MOMENTUM, BOSONS, COMPOSITE MODELS, DISTANCE, ELECTRIC FIELDS, ELEMENTARY PARTICLES, ENERGY RANGE, EQUATIONS, FUNCTIONS, HADRONS, INTEGRAL EQUATIONS, LIE GROUPS, MANY-BODY PROBLEM, MATHEMATICAL MODELS, MESON RESONANCES, MESONS, PARTICLE MODELS, PARTICLE PROPERTIES, POINCARE GROUPS, RESONANCE PARTICLES, SYMMETRY GROUPS
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Skachkov, N.B.
Joint Inst. for Nuclear Research, Dubna (USSR). Lab. of Theoretical Physics1974
Joint Inst. for Nuclear Research, Dubna (USSR). Lab. of Theoretical Physics1974
AbstractAbstract
No abstract available
Primary Subject
Secondary Subject
Source
1974; 26 p; 17 refs.; 2 figs.
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Report
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Skachkov, N.B.
Joint Inst. for Nuclear Research, Dubna (USSR). Lab. of Theoretical Physics1981
Joint Inst. for Nuclear Research, Dubna (USSR). Lab. of Theoretical Physics1981
AbstractAbstract
[en] The relativistic equation for a system of two particles with spin 1/2 is transformed to a local form in the Lobachevsky momentum space. With the help of the expansion over unitary irreducible representations of the Lorentz group the equation is transformed to a differential-difference equation
[ru]
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1981; 14 p; 21 refs.; submitted to the journal Theor. Math. Phys.
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Skachkov, N.B.
Joint Inst. for Nuclear Research, Dubna (USSR). Lab. of Theoretical Physics1990
Joint Inst. for Nuclear Research, Dubna (USSR). Lab. of Theoretical Physics1990
AbstractAbstract
[en] In the present paper, physical arguments are given in favour of measuring the fragmentation functions Dq-h(z,s) in the process e+e-→h+X(h-π, K, p is an identified hadron, X stands for all others) at LEP energies. It is shown that due to the QCD prediction of strong scaling violation in the region of time-like momentum transfers q (q2>0, the channel of the lepton-antilepton annihilation into the hadrons, q2=S), that is essentially more strong than the analogous effect in the space-like region (q2<0, the deep-inelastic lepton-hadron scattering channel, - q2=Q2>0), the study of these fragmentation functions is of great interest. The measurement of the forward-backward asymmetry for hadrons produced in the reaction e+e-→h+X will make it possible to determine the W3(z,s) structure function that contains the contribution of the neutral quark currents leading to the parity-violation effects. 35 refs.; 8 figs.; 1 tab
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1990; 15 p
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Report
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ANNIHILATION, DEEP INELASTIC SCATTERING, DIFFERENTIAL CROSS SECTIONS, ELECTRON-POSITRON INTERACTIONS, ELECTRON-PROTON INTERACTIONS, ENERGY DEPENDENCE, FEYNMAN DIAGRAM, FOUR MOMENTUM TRANSFER, GEV RANGE, HADRONS, INCLUSIVE INTERACTIONS, KAONS, PARTICLE PRODUCTION, PIONS, PROTONS, QUARKS, SCALE INVARIANCE, STRUCTURE FUNCTIONS
BARYONS, BOSONS, CATIONS, CHARGED PARTICLES, CROSS SECTIONS, DIAGRAMS, ELECTRON-NUCLEON INTERACTIONS, ELEMENTARY PARTICLES, ENERGY RANGE, FERMIONS, FUNCTIONS, HYDROGEN IONS, HYDROGEN IONS 1 PLUS, INELASTIC SCATTERING, INFORMATION, INTERACTIONS, INVARIANCE PRINCIPLES, IONS, LEPTON-BARYON INTERACTIONS, LEPTON-HADRON INTERACTIONS, LEPTON-LEPTON INTERACTIONS, LEPTON-NUCLEON INTERACTIONS, MESONS, MOMENTUM TRANSFER, NUCLEONS, PARTICLE INTERACTIONS, POSTULATED PARTICLES, PSEUDOSCALAR MESONS, SCATTERING, STRANGE MESONS, STRANGE PARTICLES
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Skachkov, N.B.
Joint Inst. for Nuclear Research, Dubna (USSR)1976
Joint Inst. for Nuclear Research, Dubna (USSR)1976
AbstractAbstract
[en] The relative motion of quarks is described in the relativistic coordinate space introduced by use of the wave function expansion on the Lorentz group. It is shown that if one includes in this expansion the supplementary series of the unitary representations of the Lorentz groups there naturally appear the potentials that confine quarks
Primary Subject
Source
1976; 8 p; 7 refs.; 1 fig.; submitted to the journal JETF Lett. and to the 18. Int. Conf. of High Energy Physics, Tbilisi (USSR).
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