1,314 research outputs found

    On a Possibility to Determine the Sign of the Polarized Gluon Distribution

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    We investigate the possibility to draw conclusions on the sign of the spin-dependent gluon distribution, ΔG(x,Q2)\Delta G(x, Q^2), from existing polarized DIS data. The spin-dependent parton distributions Δuv,Δdv,Δuˉ,Δdˉ,Δs\Delta u_v, \Delta d_v, \Delta {\bar u}, \Delta {\bar d}, \Delta {s}, and ΔG\Delta G are constructed in the framework of a phenomenological procedure taking into account some assumptions on signs of valence and sea parton distributions motivated by 't Hooft's mechanism of quark-quark interaction induced by instantons. The axial gluon anomaly and data on integral quark contributions to the proton spin, Δu~,Δd~\Delta \tilde u, \Delta \tilde d, and Δs~\Delta \tilde s, are also taken into account. Predictions for the xx- and Q2Q^2-dependencies of the polarized proton and neutron structure functions, g1pg_1^p and g1ng_1^n, are compared to experimental data. It is shown that the neutron structure function, g1ng_1^n, is especially sensitive to the sign of ΔG(x,Q2)\Delta G(x, Q^2). The results of our analysis supports the conclusion that this sign should be positive.Comment: 14 pages, latex, 12 figure

    Is there still a strong CP problem?

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    The role of a chiral U(1) phase in the quark mass in QCD is analysed from first principles. In operator formulation, there is a parity symmetry and the phase can be removed by a change in the representation of the Dirac gamma matrices. Moreover, these properties are also realized in a Pauli-Villars regularized version of the theory. In the functional integral scenario, attempts to remove the chiral phase by a chiral transformation are thought to be obstructed by a nontrivial Jacobian arising from the fermion measure and the chiral phase may therefore seem to break parity. But if one starts from the regularized action with the chiral phase also present in the regulator mass term, the Jacobian for a combined chiral rotation of quarks and regulators is seen to be trivial and the phase can be removed by a combined chiral rotation. This amounts to a taming of the strong CP problem.Comment: 6 pages, REVTeX; brief discussion available at http://theory.saha.ernet.in/~mitra/scp.htm

    Jet Energy Density in Hadron-Hadron Collisions at High Energies

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    The average particle multiplicity density dN/deta is the dynamical quantity which reflects some regularities of particle production in low-pT range. The quantity is an important ingredient of z-scaling. Experimental results on charged particle density are available for pp, pA and AA collisions while experimental properties of the jet density are still an open question. The goal of this work is to find the variable which will reflect the main features of the jet production in low transverse energy range and play the role of the scale factor for the scaling function psi(z) and variable z in data z-presentation. The appropriate candidate is the variable we called "scaled jet energy density". Scaled jet energy density is the probability to have a jet with defined ET in defined xT and pseudorapidity regions. The PYTHIA6.2 Monte Carlo generator is used for calculation of scaled jet energy density in proton-proton collisions over a high energy range (sqrt s = 200-14000 GeV) and at eta = 0. The properties of the new variable are discussed and sensitivity to "physical scenarios" applied in the standard Monte Carlo generator is noted. The results of scaled jet energy density at LHC energies are presented and compared with predictions based on z-scaling.Comment: 11 pages, LaTeX, 8 figures, Presented at the XVII International Baldin Seminar on High Energy Physics Problems "Relativistic Nuclear Physics & Quantum Chromodynamics", Dubna, Russia, September 27 - October 2, 200

    Criminal protection of rights and legal interests of minors

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    Π’ ΡΡ‚Π°Ρ‚ΡŒΠ΅ Ρ€Π°ΡΡΠΌΠ°Ρ‚Ρ€ΠΈΠ²Π°ΡŽΡ‚ΡΡ особСнности ΠΊΠ²Π°Π»ΠΈΡ„ΠΈΠΊΠ°Ρ†ΠΈΠΈ общСствСнно-опасного дСяния Π² Π²ΠΈΠ΄Π΅ Π½Π΅ΠΎΠ΄Π½ΠΎΠΊΡ€Π°Ρ‚Π½ΠΎΠΉ Ρ€ΠΎΠ·Π½ΠΈΡ‡Π½ΠΎΠΉ ΠΏΡ€ΠΎΠ΄Π°ΠΆΠΈ алкогольной ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ†ΠΈΠΈ Π½Π΅ΡΠΎΠ²Π΅Ρ€ΡˆΠ΅Π½Π½ΠΎΠ»Π΅Ρ‚Π½ΠΈΠΌ.The article is devoted to the analysis of the specialties of qualification of the socially dangerous act like repeated retail sale of alcoholic products to minors

    Permafrost hydrology in changing climatic conditions: seasonal variability of stable isotope composition in rivers in discontinuous permafrost

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    Role of changing climatic conditions on permafrost degradation and hydrology was investigated in the transition zone between the tundra and forest ecotones at the boundary of continuous and discontinuous permafrost of the lower Yenisei River. Three watersheds of various sizes were chosen to represent the characteristics of the regional landscape conditions. Samples of river flow, precipitation, snow cover, and permafrost ground ice were collected over the watersheds to determine isotopic composition of potential sources of water in a river flow over a two year period. Increases in air temperature over the last forty years have resulted in permafrost degradation and a decrease in the seasonal frost which is evident from soil temperature measurements, permafrost and active-layer monitoring, and analysis of satellite imagery. The lowering of the permafrost table has led to an increased storage capacity of permafrost affected soils and a higher contribution of ground water to river discharge during winter months. A progressive decrease in the thickness of the layer of seasonal freezing allows more water storage and pathways for water during the winter low period making winter discharge dependent on the timing and amount of late summer precipitation. There is a substantial seasonal variability of stable isotopic composition of river flow. Spring flooding corresponds to the isotopic composition of snow cover prior to the snowmelt. Isotopic composition of river flow during the summer period follows the variability of precipitation in smaller creeks, while the water flow of larger watersheds is influenced by the secondary evaporation of water temporarily stored in thermokarst lakes and bogs. Late summer precipitation determines the isotopic composition of texture ice within the active layer in tundra landscapes and the seasonal freezing layer in forested landscapes as well as the composition of the water flow during winter months

    Photon Physics in Heavy Ion Collisions at the LHC

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    Various pion and photon production mechanisms in high-energy nuclear collisions at RHIC and LHC are discussed. Comparison with RHIC data is done whenever possible. The prospect of using electromagnetic probes to characterize quark-gluon plasma formation is assessed.Comment: Writeup of the working group "Photon Physics" for the CERN Yellow Report on "Hard Probes in Heavy Ion Collisions at the LHC", 134 pages. One figure added in chapter 5 (comparison with PHENIX data). Some figures and correponding text corrected in chapter 6 (off-chemical equilibrium thermal photon rates). Some figures modified in chapter 7 (off-chemical equilibrium photon rates) and comparison with PHENIX data adde

    ΠšΠ°Ρ‡Π΅ΡΡ‚Π²Π΅Π½Π½Π°Ρ ΠΈ количСствСнная ΠΎΡ†Π΅Π½ΠΊΠ° Π»ΠΈΠΊΠ²ΠΎΡ€ΠΎΠ΄ΠΈΠ½Π°ΠΌΠΈΠΊΠΈ

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    Disorders of cerebrospinal fluid (CSF) secretion, dynamics and absorption are common in different illnesses and injuries of the central nervous system (CNS). Nowadays magnetic-resonance tomography (MRI) is the leading research method of CSF dynamics. There are some MRI techniques for both qualitative and quantitative evaluation of CSF dynamic. The assessment of CSF movement is needed to define treatment strategy for patients with different types of hydrocephalus. In this review we have summarized the information about physic basement, area of application of modern MRI techniques. The main attention was paid to modern views on hydrocephalus pathogenesis, pathological CSF flow dynamics in CNS disorders and traumatic brain injury.ΠΠ°Ρ€ΡƒΡˆΠ΅Π½ΠΈΡ ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ†ΠΈΠΈ, Ρ‚ΠΎΠΊΠ° ΠΈ Ρ€Π΅Π·ΠΎΡ€Π±Ρ†ΠΈΠΈ спинномозговой Тидкости (Π‘ΠœΠ–) Π²ΡΡ‚Ρ€Π΅Ρ‡Π°ΡŽΡ‚ΡΡ ΠΏΡ€ΠΈ ΠΌΠ½ΠΎΠ³ΠΈΡ… заболСваниях ΠΈ поврСТдСниях Π½Π΅Ρ€Π²Π½ΠΎΠΉ систСмы. Π’ настоящСС врСмя ΠΌΠ°Π³Π½ΠΈΡ‚Π½ΠΎ-рСзонансная томография (МРВ) являСтся Π²Π΅Π΄ΡƒΡ‰ΠΈΠΌ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ исслСдования Π»ΠΈΠΊΠΎΠ²ΠΎΡ€ΠΎΠ΄ΠΈΠ½Π°ΠΌΠΈΠΊΠΈ. На сСгодняшний дСнь извСстно нСсколько ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΈΠΊ исслСдования, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡŽΡ‚ ΠΎΡ†Π΅Π½ΠΈΡ‚ΡŒ качСствСнныС ΠΈ количСствСнныС ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Ρ‹ двиТСния спинномозговой Тидкости. ΠžΡ†Π΅Π½ΠΊΠ° Π»ΠΈΠΊΠ²ΠΎΡ€ΠΎΠ΄ΠΈΠ½Π°ΠΌΠΈΠΊΠΈ Π½Π΅ΠΎΠ±Ρ…ΠΎΠ΄ΠΈΠΌΠ° для опрСдСлСния ΠΏΡ€Π°Π²ΠΈΠ»ΡŒΠ½ΠΎΠΉ Ρ‚Π°ΠΊΡ‚ΠΈΠΊΠΈ лСчСния ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ² с Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹ΠΌΠΈ Π²ΠΈΠ΄Π°ΠΌΠΈ Π³ΠΈΠ΄Ρ€ΠΎΡ†Π΅Ρ„Π°Π»ΠΈΠΈ. Π’ ΠΎΠ±Π·ΠΎΡ€Π΅ Π»ΠΈΡ‚Π΅Ρ€Π°Ρ‚ΡƒΡ€Ρ‹ ΠΏΡ€ΠΈΠ²Π΅Π΄Π΅Π½Ρ‹ физичСскиС основы, области примСнСния соврСмСнных МРВ-ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠ² изучСния Π»ΠΈΠΊΠ²ΠΎΡ€ΠΎΠ΄ΠΈΠ½Π°ΠΌΠΈΠΊΠΈ. ОсобоС Π²Π½ΠΈΠΌΠ°Π½ΠΈΠ΅ ΡƒΠ΄Π΅Π»Π΅Π½ΠΎ соврСмСнным взглядам Π½Π° ΠΏΠ°Ρ‚ΠΎΠ³Π΅Π½Π΅Π· Π³ΠΈΠ΄Ρ€ΠΎΡ†Π΅Ρ„Π°Π»ΠΈΠΈ, особСнностям Ρ‚ΠΎΠΊΠ° Π»ΠΈΠΊΠ²ΠΎΡ€Π° ΠΏΡ€ΠΈ Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Ρ… заболСваниях Ρ†Π΅Π½Ρ‚Ρ€Π°Π»ΡŒΠ½ΠΎΠΉ Π½Π΅Ρ€Π²Π½ΠΎΠΉ систСмы ΠΈ Ρ‡Π΅Ρ€Π΅ΠΏΠ½ΠΎ-ΠΌΠΎΠ·Π³ΠΎΠ²ΠΎΠΉ Ρ‚Ρ€Π°Π²ΠΌΠ΅
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