1,255 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

    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

    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

    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΅

    Tungstate Based Ceramics Obtained By Spark Plasma Sintering Method – Possible Material for Consolidation of Radioactive Wastes’ Components

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    The Spark Plasma Sintering method was used to produce high-density ceramics from tungstates SrWO4 and NaNd(WO4)2 with scheelite structure. These compounds are proposed as possible matrices for the consolidation of radwaste components. Powder samples were obtained by coprecipitation method and studied by X-ray diffraction analysis (XRD) and scanning electron microscopy (SEM). After sintering, the samples retained their phase identity (scheelite structure). The total duration of sintering was ∼ 13-15 min, the relative density was reached ∼ 92, 99%. Keywords: Tungstates, RW, Spark Plasma Sintering, high density, microstructur

    The Gross--Llewellyn Smith Sum Rule in the Analytic Approach to Perturbative QCD

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    We apply analytic perturbation theory to the Gross--Llewellyn Smith sum rule. We study the Q2Q^2 evolution and the renormalization scheme dependence of the analytic three-loop QCD correction to this sum rule, and demonstrate that the results are practically renormalization scheme independent and lead to rather different Q2Q^2 evolution than the standard perturbative correction possesses.Comment: 17 pages, 9 eps figures, REVTe

    РадиохирургичСскоС Π»Π΅Ρ‡Π΅Π½ΠΈΠ΅ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚Π° с Ρ€Π°Π·Ρ€Ρ‹Π²ΠΎΠΌ Π°Ρ€Ρ‚Π΅Ρ€ΠΈΠΎΠ²Π΅Π½ΠΎΠ·Π½ΠΎΠΉ ΠΌΠ°Π»ΡŒΡ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈΠΈ, располоТСнной Π² Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΎΠ½Π°Π»ΡŒΠ½ΠΎ Π·Π½Π°Ρ‡ΠΈΠΌΠΎΠΉ Π·ΠΎΠ½Π΅

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    Arteriovenous malformations (AVMs) of the brain are quite rare vascular pathologies, but they are life-threatening, due to the risk of intracerebral hemorrhage. Stereotactic radiosurgical treatment of patients with cerebral AVM is performed in cases where surgical removal is impossible or embolization with a stable occlusive effect cannot be performed. Currently, for the diagnosis of AVM, magnetic resonance imaging (MRI) is increasingly used because of its noninvasiveness and minimal risks. When a malformation is located in a functionally significant area, then a non-invasive technique is used to assess its interposition and mapping - functional magnetic resonance imaging.We have presented the experience of radiosurgical treatment of a 43-year-old male patient with a ruptured AVM located in the left temporal lobe, near Wernicke’s area. The patient underwent stereotactic radiosurgical treatment with Elekta Leksell Gamma Knife Perfection device, taking into account the location of the AVM in a functionally significant area, preoperative mapping was performed. After two years, according to MR angiography, the arterial component in the projection of the irradiated AVM was not visualized, which was confirmed by the data of cerebral angiography. Thus, a clinical example has demonstrated the high efficiency of MRI in the diagnosis and assessment of the results of the performed stereotactic radiosurgical treatment of AVMs. АртСриовСнозныС ΠΌΠ°Π»ΡŒΡ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈΠΈ (ΠΠ’Πœ) Π³ΠΎΠ»ΠΎΠ²Π½ΠΎΠ³ΠΎ ΠΌΠΎΠ·Π³Π° β€” достаточно Ρ€Π΅Π΄ΠΊΠΈΠ΅ сосудистыС ΠΏΠ°Ρ‚ΠΎΠ»ΠΎΠ³ΠΈΠΈ, ΠΎΠ΄Π½Π°ΠΊΠΎ ΡΠ²Π»ΡΡŽΡ‚ΡΡ опасными для ΠΆΠΈΠ·Π½ΠΈ Π² связи с риском развития Π²Π½ΡƒΡ‚Ρ€ΠΈΠΌΠΎΠ·Π³ΠΎΠ²ΠΎΠ³ΠΎ кровоизлияния. БтСрСотаксичСскоС радиохирургичСскоС Π»Π΅Ρ‡Π΅Π½ΠΈΠ΅ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ² с ΠΠ’Πœ Π³ΠΎΠ»ΠΎΠ²Π½ΠΎΠ³ΠΎ ΠΌΠΎΠ·Π³Π° ΠΏΡ€ΠΈΠΌΠ΅Π½ΡΡŽΡ‚ Π² Ρ‚Π΅Ρ… случаях, ΠΊΠΎΠ³Π΄Π° ΡƒΠ΄Π°Π»Π΅Π½ΠΈΠ΅ хирургичСским способом Π½Π΅ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎ ΠΈΠ»ΠΈ Π½Π΅ ΠΌΠΎΠΆΠ΅Ρ‚ Π±Ρ‹Ρ‚ΡŒ ΠΏΡ€ΠΎΠ²Π΅Π΄Π΅Π½Π° эмболизация с устойчивым ΠΎΠΊΠΊΠ»ΡŽΠ·ΠΈΠΎΠ½Π½Ρ‹ΠΌ эффСктом. Π’ настоящСС врСмя для диагностики ΠΠ’Πœ всС Ρ‡Π°Ρ‰Π΅ ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΡƒΡŽΡ‚ ΠΌΠ°Π³Π½ΠΈΡ‚Π½ΠΎ-Ρ€Π΅Π·ΠΎΠ½Π°Π½ΡΠ½ΡƒΡŽ Ρ‚ΠΎΠΌΠΎΠ³Ρ€Π°Ρ„ΠΈΡŽ (МРВ) ΠΈΠ·-Π·Π° Π΅Π΅ нСинвазивности ΠΈ ΠΌΠΈΠ½ΠΈΠΌΠ°Π»ΡŒΠ½Ρ‹Ρ… рисков. ΠŸΡ€ΠΈ располоТСнии ΠΌΠ°Π»ΡŒΡ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈΠΈ Π² Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΎΠ½Π°Π»ΡŒΠ½ΠΎ Π·Π½Π°Ρ‡ΠΈΠΌΠΎΠΉ Π·ΠΎΠ½Π΅ для ΠΎΡ†Π΅Π½ΠΊΠΈ Π΅Π΅ взаиморасполоТСния ΠΈ картирования ΠΏΡ€ΠΈΠΌΠ΅Π½ΡΡŽΡ‚ Π½Π΅ΠΈΠ½Π²Π°Π·ΠΈΠ²Π½ΡƒΡŽ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΈΠΊΡƒ β€” Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΎΠ½Π°Π»ΡŒΠ½ΡƒΡŽ МРВ.Нами прСдставлСн ΠΎΠΏΡ‹Ρ‚ радиохирургичСского лСчСния ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚Π° 43 Π»Π΅Ρ‚ с Ρ€Π°Π·Ρ€Ρ‹Π²ΠΎΠΌ ΠΠ’Πœ, располоТСнной Π² Π»Π΅Π²ΠΎΠΉ височной Π΄ΠΎΠ»Π΅, Π²Π±Π»ΠΈΠ·ΠΈ Π·ΠΎΠ½Ρ‹ Π’Π΅Ρ€Π½ΠΈΠΊΠ΅. Π‘ΠΎΠ»ΡŒΠ½ΠΎΠΌΡƒ Π±Ρ‹Π»ΠΎ ΠΏΡ€ΠΎΠ²Π΅Π΄Π΅Π½ΠΎ стСрСотаксичСскоС радиохирургичСскоС Π»Π΅Ρ‡Π΅Π½ΠΈΠ΅ Π½Π° Π°ΠΏΠΏΠ°Ρ€Π°Ρ‚Π΅ β€œElekta Leksell Gamma Knife Perfection”, с ΡƒΡ‡Π΅Ρ‚ΠΎΠΌ располоТСния ΠΠ’Πœ Π² Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΎΠ½Π°Π»ΡŒΠ½ΠΎ Π·Π½Π°Ρ‡ΠΈΠΌΠΎΠΉ Π·ΠΎΠ½Π΅, Π²Ρ‹ΠΏΠΎΠ»Π½ΠΈΠ»ΠΈ ΠΏΡ€Π΅Π΄ΠΎΠΏΠ΅Ρ€Π°Ρ†ΠΈΠΎΠ½Π½ΠΎΠ΅ ΠΊΠ°Ρ€Ρ‚ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅. По ΠΏΡ€ΠΎΡˆΠ΅ΡΡ‚Π²ΠΈΠΈ Π΄Π²ΡƒΡ… Π»Π΅Ρ‚ ΠΏΠΎ Π΄Π°Π½Π½Ρ‹ΠΌ МР-Π°Π½Π³ΠΈΠΎΠ³Ρ€Π°Ρ„ΠΈΠΈ Π°Ρ€Ρ‚Π΅Ρ€ΠΈΠ°Π»ΡŒΠ½Ρ‹ΠΉ ΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚ Π² ΠΏΡ€ΠΎΠ΅ΠΊΡ†ΠΈΠΈ ΠΎΠ±Π»ΡƒΡ‡Π΅Π½Π½ΠΎΠΉ ΠΠ’Πœ Π½Π΅ визуализировался, Ρ‡Ρ‚ΠΎ ΠΏΠΎΠ΄Ρ‚Π²Π΅Ρ€ΠΆΠ΄Π°Π»ΠΎΡΡŒ Π΄Π°Π½Π½Ρ‹ΠΌΠΈ Ρ†Π΅Ρ€Π΅Π±Ρ€Π°Π»ΡŒΠ½ΠΎΠΉ Π°Π½Π³ΠΈΠΎΠ³Ρ€Π°Ρ„ΠΈΠΈ. Π’Π°ΠΊΠΈΠΌ ΠΎΠ±Ρ€Π°Π·ΠΎΠΌ, Π½Π° клиничСском ΠΏΡ€ΠΈΠΌΠ΅Ρ€Π΅ продСмонстрирована высокая ΡΡ„Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒ МРВ Π² диагностикС ΠΈ ΠΎΡ†Π΅Π½ΠΊΠ΅ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΎΠ² ΠΏΡ€ΠΎΠ²Π΅Π΄Π΅Π½Π½ΠΎΠ³ΠΎ стСрСотаксичСского радиохирургичСского лСчСния ΠΠ’Πœ.

    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
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