38 research outputs found

    Parametric down conversion of X-ray photons

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    Energy, Hamiltonian, Noether Charge, and Black Holes

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    It is shown that in general the energy E{\cal E} and the Hamiltonian H{\cal H} of matter fields on the black hole exterior play different roles. H{\cal H} is a generator of the time evolution along the Killing time while E{\cal E} enters the first law of black hole thermodynamics. For non-minimally coupled fields the difference Hβˆ’E{\cal H}-{\cal E} is not zero and is a Noether charge QQ analogous to that introduced by Wald to define the black hole entropy. If fields vanish at the spatial boundary, QQ is reduced to an integral over the horizon. The analysis is carried out and an explicit expression for QQ is found for general diffeomorphism invariant theories. As an extension of the results by Wald et al, the first law of black hole thermodynamics is derived for arbitrary weak matter fields.Comment: 20 pages, latex, no figure

    Application of the Large-N_c limit to a Chiral Lagrangian with Resonances

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    It is shown that the implementation of the Large--NcN_c approximation helps to get insight into the structure of, in principle, any QCD-like theory. As an example, we will compute the NLO corrections to L10L_{10} in the chiral limit with a Lagrangian with Resonances.Comment: 9 pages, 1 figure. Talk given at the International School of Subnuclear Physics (Erice 2002). To be published in the Proceeding

    Impact of Electrical Current on Single GaAs Nanowire Structure

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    The impact of electrical current on the structure of single free-standing Be-doped GaAs nanowires grown on a Si 111 substrate is investigated. Single nanowires have been structurally analyzed by X-ray nanodiffraction using synchrotron radiation before and after the application of an electrical current. The conductivity measurements on single nanowires in their as-grown geometry have been realized via W-probes installed inside a dual-beam focused ion beam/scanning electron microscopy chamber. Comparing reciprocal space maps of the 111 Bragg reflection, extracted perpendicular to the nanowire growth axis before and after the conductivity measurement, the structural impact of the electrical current is evidenced, including deformation of the hexagonal nanowire cross section, tilting, and bending with respect to the substrate normal. For electrical current densities below 30 A mmβˆ’2, the induced changes in the reciprocal space maps are negligible. However, for a current density of 347 A mmβˆ’2, the diffraction pattern is completely distorted. The mean cross section of the illuminated nanowire volume is reconstructed from the reciprocal space maps before and after the application of electrical current. Interestingly, the elongation of two pairs of opposing side facets accompanied by shrinkage of the third pair of facets is found. The variations in the nanowire diameter, as well as their tilt and bending, are confirmed by scanning electron microscopy. To explain these findings, material melting due to Joule heating during voltage/current application accompanied by anisotropic deformations induced by the W-probe is suggested

    QCD Instantons and the Soft Pomeron

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    We study the role of semi-classical QCD vacuum solutions in high energy scattering by considering the instanton contribution to hadronic cross sections. We propose a new type of instanton-induced interactions (``instanton ladder'') that leads to the rising with energy hadronic cross section of Regge type (the Pomeron). We argue that this interaction may be responsible for the structure of the soft Pomeron. The intercept is calculated. It has a non-analytic dependence on the strong coupling constant, allowing a non-singular continuation into the non-perturbative region. We derive the Pomeron trajectory, which appears to be approximately linear in some range of (negative) momentum transfer t, but exhibits a curvature at small t. Possible role of instantons in multiparticle production is also discussed.Comment: 20 pages, 8 figures, ReVTe

    Instantons in the Saturation Environment

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    We show that instanton calculations in QCD become theoretically well defined in the gluon saturation environment which suppresses large size instantons. The effective cutoff scale is determined by the inverse of the saturation scale. We concentrate on two most important cases: the small-x tail of a gluon distribution of a high energy hadron or a large nucleus and the central rapidity region in a high energy hadronic or heavy ion collision. In the saturation regime the gluon density in a single large ultrarelativistic nucleus is high and gluonic fields are given by the classical solutions of the equations of motion. We show that these strong classical fields do not affect the density of instantons in the nuclear wave function compared to the instanton density in the vacuum. A classical solution with non-trivial topological charge is found for the gluon field of a single nucleus at the lowest order in the instanton perturbation theory. In the case of ultrarelativistic heavy ion collisions a strong classical gluonic field is produced in the central rapidity region. We demonstrate that this field introduces a suppression factor of exp{-c \rho^4 Q_s^4 / [8 \alpha^2 N_c (Q_s \tau)^2]} in the instanton size distribution, where Q_s is the saturation scale of both (identical) nuclei, \tau is the proper time and c = 1 is the gluon liberation coefficient. This factor suggests that gluonic saturation effects at the early stages of nuclear collisions regulate the instanton size distribution in the infrared region and make the instanton density finite by suppressing large size instantons.Comment: 20 pages, 8 figures, REVTeX, some discussion added including a possible scenario for unitarization of the soft pomero

    Π˜ΠΌΠΌΡƒΠ½ΠΎΠ»ΠΎΠ³ΠΈΡ‡Π΅ΡΠΊΠΈΠ΅ эффСкты Π°Π΄Π°Π»ΠΈΠΌΡƒΠΌΠ°Π±Π° ΠΏΡ€ΠΈ Ρ€Π΅Π²ΠΌΠ°Ρ‚ΠΎΠΈΠ΄Π½ΠΎΠΌ Π°Ρ€Ρ‚Ρ€ΠΈΡ‚Π΅: Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ Российского Π½Π°Ρ†ΠΈΠΎΠ½Π°Π»ΡŒΠ½ΠΎΠ³ΠΎ исслСдования

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    A reduction in immunological parameters during therapy for rheumatoid arthritis (RA) can yield new data on the mechanisms of anti-inflammatory action and be of great practical importance since this allows judgment of the depth of impact on the immunological process and therefore may be regarded as one of the components of improvement and remission. Objective: to study the effect of the tumor necrosis factor-a (TNF-Π°) inhibitor adalimumab (ADA) on a number of key immunological parameters in RA. Subjects and methods. The study included 100 patients (11 men and 89 women) diagnosed with RA from 5 research centers. The patients were observed to have high RA activity: at baseline, DAS28 6.22+0.84 scores; C-reactive protein (CRP) 37.1+34.7 mg/l. The mean number of disease-modifying antirheumatic drugs (DMARDs) used by a patient in the history was 2.1. During 24-week treatment, the patients took ADA in a subcutaneous dose of 40 mg every 2 weeks both alone and in combination with DMARDs. The time course of changes in the serum levels of CRP, IGM rheumatoid factor (RF) and in the concentration of anti-cyclic citrullinated peptide 2 (anti-CCP2) antibodies was determined by enzyme immunoassay (EIA) using the Axis-Shield Diagnostics commercial kits (United Kingdom). The levels of TNF-a, interleukin (IL) 6, 12, matrix metalloproteinase 3 (MMP3) were measured in pg/ml by EIA using the Bender MedSystems commercial kits (USA) according to the manufacturer's directions. Results. During ADA therapy, there was a rapid reduction in the level of CRP from 34.3 to 11.317.2 mg/l following 2 weeks (p<0.001), which thereafter remained low (11.9 mg/l), with some fluctuations, until week 24 of the study. There was a significant reduction in blood RF levels from 169.24 to 111.97 at 24 weeks (p<0.001). After 12 weeks of ADA treatment, there was virtually a two-fold decrease in IL-6 content from 8.87 to 4.87 pg/ml and later on to 4.03 pg/ml at week 24 (p>0,05). The mean levels of anti-CCP2 antibodies, IL-12, VEGF, and MMP3 remained unchanged. Conclusion. The time course of changes in immunological parameters during ADA treatment demonstrates the rapid and deep effect of TNF-a inhibitors on the different components of the pathogenesis of RA.Π‘Π½ΠΈΠΆΠ΅Π½ΠΈΠ΅ иммунологичСских ΠΏΠΎΠΊΠ°Π·Π°Ρ‚Π΅Π»Π΅ΠΉ Π½Π° Ρ„ΠΎΠ½Π΅ Ρ‚Π΅Ρ€Π°ΠΏΠΈΠΈ Ρ€Π΅Π²ΠΌΠ°Ρ‚ΠΎΠΈΠ΄Π½ΠΎΠ³ΠΎ Π°Ρ€Ρ‚Ρ€ΠΈΡ‚Π° (РА) позволяСт ΠΏΠΎΠ»ΡƒΡ‡ΠΈΡ‚ΡŒ Π½ΠΎΠ²Ρ‹Π΅ Π΄Π°Π½Π½Ρ‹Π΅ ΠΎ ΠΌΠ΅Ρ…Π°Π½ΠΈΠ·ΠΌΠ°Ρ… ΠΏΡ€ΠΎΡ‚ΠΈΠ²ΠΎΠ²ΠΎΡΠΏΠ°Π»ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠ³ΠΎ дСйствия ΠΈ ΠΈΠΌΠ΅Π΅Ρ‚ Π²Π°ΠΆΠ½ΠΎΠ΅ практичСскоС Π·Π½Π°Ρ‡Π΅Π½ΠΈΠ΅, ΠΏΠΎΡΠΊΠΎΠ»ΡŒΠΊΡƒ позволяСт ΡΡƒΠ΄ΠΈΡ‚ΡŒ ΠΎ Π³Π»ΡƒΠ±ΠΈΠ½Π΅ воздСйствия Π½Π° иммунопатологичСский процСсс ΠΈ поэтому ΠΌΠΎΠΆΠ΅Ρ‚ ΠΎΡ†Π΅Π½ΠΈΠ²Π°Ρ‚ΡŒΡΡ ΠΊΠ°ΠΊ ΠΎΠ΄ΠΈΠ½ ΠΈΠ· ΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚ΠΎΠ² ΡƒΠ»ΡƒΡ‡ΡˆΠ΅Π½ΠΈΡ ΠΈ рСмиссии. ЦСль исслСдования β€” ΠΈΠ·ΡƒΡ‡Π΅Π½ΠΈΠ΅ влияния ΠΈΠ½Π³ΠΈΠ±ΠΈΡ‚ΠΎΡ€Π° Ρ„Π°ΠΊΡ‚ΠΎΡ€Π° Π½Π΅ΠΊΡ€ΠΎΠ·Π° ΠΎΠΏΡƒΡ…ΠΎΠ»ΠΈ Ξ± (ЀНОα) Π°Π΄Π°Π»ΠΈΠΌΡƒΠΌΠ°Π±Π° (АДА) Π½Π° ряд ΠΊΠ»ΡŽΡ‡Π΅Π²Ρ‹Ρ… иммунологичСских ΠΏΠΎΠΊΠ°Π·Π°Ρ‚Π΅Π»Π΅ΠΉ ΠΏΡ€ΠΈ РА. ΠœΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π» ΠΈ ΠΌΠ΅Ρ‚ΠΎΠ΄Ρ‹. Π’ исслСдованиС Π²ΠΊΠ»ΡŽΡ‡Π΅Π½ΠΎ 100 ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ² ΠΈΠ· 5 ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Ρ‚Π΅Π»ΡŒΡΠΊΠΈΡ… Ρ†Π΅Π½Ρ‚Ρ€ΠΎΠ² с Π΄ΠΈΠ°Π³Π½ΠΎΠ·ΠΎΠΌ РА (11 ΠΌΡƒΠΆΡ‡ΠΈΠ½ ΠΈ 89 ΠΆΠ΅Π½Ρ‰ΠΈΠ½). Π£ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ² наблюдалась высокая Π°ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒ РА: исходно индСкс DAS28 β€” 6,22Β±0,84 Π±Π°Π»Π»Π°, ΡƒΡ€ΠΎΠ²Π΅Π½ΡŒ Π‘-Ρ€Π΅Π°ΠΊΡ‚ΠΈΠ²Π½ΠΎΠ³ΠΎ Π±Π΅Π»ΠΊΠ° (Π‘Π Π‘) β€” 37,1+34,7ΠΌΠ³/Π». Π‘Ρ€Π΅Π΄Π½Π΅Π΅ число базисных ΠΏΡ€ΠΎΡ‚ΠΈΠ²ΠΎΠ²ΠΎΡΠΏΠ°Π»ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… ΠΏΡ€Π΅ΠΏΠ°Ρ€Π°Ρ‚ΠΎΠ² (Π‘ΠŸΠ’ΠŸ) Π² Π°Π½Π°ΠΌΠ½Π΅Π·Π΅, ΠΏΡ€ΠΈΠΌΠ΅Π½ΡΠ²ΡˆΠΈΡ…ΡΡ ΠΎΠ΄Π½ΠΈΠΌ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠΌ, составило 2,1. Π—Π° врСмя лСчСния (24 Π½Π΅Π΄) ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚Ρ‹ ΠΏΠΎΠ»ΡƒΡ‡Π°Π»ΠΈ АДА Π² Π΄ΠΎΠ·Π΅ 40 ΠΌΠ³ ΠΊΠ°ΠΆΠ΄Ρ‹Π΅ 2 Π½Π΅Π΄ ΠΏΠΎΠ΄ΠΊΠΎΠΆΠ½ΠΎ ΠΊΠ°ΠΊ Π² ΠΊΠΎΠΌΠ±ΠΈΠ½Π°Ρ†ΠΈΠΈ с Π‘ΠŸΠ’ΠŸ, Ρ‚Π°ΠΊ ΠΈ Π² ΠΌΠΎΠ½ΠΎΡ‚Π΅Ρ€Π°ΠΏΠΈΠΈ. ΠžΠΏΡ€Π΅Π΄Π΅Π»ΡΠ»ΠΈ Π² Π΄ΠΈΠ½Π°ΠΌΠΈΠΊΠ΅ сывороточныС ΡƒΡ€ΠΎΠ²Π½ΠΈ Π‘Π Π‘, IgM Ρ€Π΅Π²ΠΌΠ°Ρ‚ΠΎΠΈΠ΄Π½ΠΎΠ³ΠΎ Ρ„Π°ΠΊΡ‚ΠΎΡ€Π° (Π Π€), ΠΊΠΎΠ½Ρ†Π΅Π½Ρ‚Ρ€Π°Ρ†ΠΈΡŽ Π°Π½Ρ‚ΠΈΡ‚Π΅Π» ΠΊ цикличСскому Ρ†ΠΈΡ‚Ρ€ΡƒΠ»Π»ΠΈΠ½ΠΈΡ€ΠΎΠ²Π°Π½Π½ΠΎΠΌΡƒ ΠΏΠ΅ΠΏΡ‚ΠΈΠ΄Ρƒ 2 (АЦЦП2) ΠΈΠ·ΡƒΡ‡Π°Π»ΠΈ ΠΈΠΌΠΌΡƒΠ½ΠΎΡ„Π΅Ρ€ΠΌΠ΅Π½Ρ‚Π½Ρ‹ΠΌ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ (ИЀМ) с ΠΏΠΎΠΌΠΎΡ‰ΡŒΡŽ коммСрчСских Π½Π°Π±ΠΎΡ€ΠΎΠ² Axis-Shield Diagnostics (ВСликобритания). Π‘ΠΎΠ΄Π΅Ρ€ΠΆΠ°Π½ΠΈΠ΅ ЀНОа, ΠΈΠ½Ρ‚Π΅Ρ€Π»Π΅ΠΉΠΊΠΈΠ½Π° (Π˜Π›) 6, 12, матриксной ΠΌΠ΅Ρ‚Π°Π»Π»ΠΎΠΏΡ€ΠΎΡ‚Π΅ΠΈΠ½Π°Π·Ρ‹ 3 (ММР3) опрСдСляли ИЀМ (Π² ΠΏΠ³/ΠΌΠ») с использованиСм коммСрчСских Π½Π°Π±ΠΎΡ€ΠΎΠ² Bender MedSystems (БША) согласно инструкциям Ρ„ΠΈΡ€ΠΌΡ‹-изготовитСля. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ исслСдования. На Ρ„ΠΎΠ½Π΅ Ρ‚Π΅Ρ€Π°ΠΏΠΈΠΈ АДА наблюдалось быстроС сниТСниС уровня Π‘Π Π‘ с 34,3 Π΄ΠΎ 11,3+17,2 ΠΌΠ³/Π» Ρ‡Π΅Ρ€Π΅Π· 2 Π½Π΅Π΄ (p<0,001), ΠΊΠΎΡ‚ΠΎΡ€Ρ‹ΠΉ Π² дальнСйшСм с Π½Π΅ΠΊΠΎΡ‚ΠΎΡ€Ρ‹ΠΌΠΈ колСбаниями оставался Π½ΠΈΠ·ΠΊΠΈΠΌ (11,9 ΠΌΠ³/Π») Π΄ΠΎ 24-ΠΉ Π½Π΅Π΄Π΅Π»ΠΈ исслСдования. Наблюдалось достовСрноС сниТСниС уровня Π Π€ Π² ΠΊΡ€ΠΎΠ²ΠΈ с 169,24 Π΄ΠΎ 111,97Π½Π° 24-ΠΉ Π½Π΅Π΄Π΅Π»Π΅ (p<0,001). Π§Π΅Ρ€Π΅Π· 12 Π½Π΅Π΄ послС Π½Π°Ρ‡Π°Π»Π° лСчСния АДА ΠΎΡ‚ΠΌΠ΅Ρ‡Π°Π»ΠΎΡΡŒ практичСски 2-ΠΊΡ€Π°Ρ‚Π½ΠΎΠ΅ сниТСниС содСрТания Π˜Π›6 с 8,87 Π΄ΠΎ 4,87 ΠΏΠ³/ΠΌΠ» ΠΈ Π² дальнСйшСм, ΠΊ 24-ΠΉ Π½Π΅Π΄Π΅Π»Π΅, β€” Π΄ΠΎ 4,03 ΠΏΠ³/ΠΌΠ» (p>0,05). Π‘Ρ€Π΅Π΄Π½ΠΈΠ΅ ΡƒΡ€ΠΎΠ²Π½ΠΈ АЦЦП, Π˜Π›12, Ρ„Π°ΠΊΡ‚ΠΎΡ€Π° роста эндотСлия сосудов (VEGF), ММП3 Π½Π΅ измСнились. Π’Ρ‹Π²ΠΎΠ΄Ρ‹. Π”ΠΈΠ½Π°ΠΌΠΈΠΊΠ° иммунологичСских ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠ² ΠΏΡ€ΠΈ Π»Π΅Ρ‡Π΅Π½ΠΈΠΈ АДА дСмонстрируСт быстроС ΠΈ Π³Π»ΡƒΠ±ΠΎΠΊΠΎΠ΅ дСйствиС ΠΈΠ½Π³ΠΈΠ±ΠΈΡ‚ΠΎΡ€ΠΎΠ² ЀНОа Π½Π° Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Π΅ звСнья ΠΏΠ°Ρ‚ΠΎΠ³Π΅Π½Π΅Π·Π° РА

    Pressure Treatment of Polytene Chromosomes and Computer Vision Techniques for High Resolution Cytogenetic Studies

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    48 p.Thesis (Ph.D.)--University of Illinois at Urbana-Champaign, 2008.The exceptional cytology provided by the interphase chromatin organization in polytene chromosomes has made Drosophila the premier model organism for analysis of chromosome structure and behavior. A major impediment to full exploitation of polytene chromosome cytology has been the difficulty in producing high quality chromosome spreads. This is particularly true for applications requiring prior formaldehyde fixation. Individual chromosome bands are seldom resolved in typical preparations, with many appearing fused. Here we describe a new procedure for preparing polytene chromosome spreads which exploits high pressure, together with other modifications, to produce high quality chromosome spreads whose light microscopy images reproducibly show comparable detail to electron microscopy images of conventionally prepared spreads. We illustrate results obtained with this procedure from typical cytological applications, including immunofluorescence and fluorescence in situ hybridization (FISH). Description of optimized downstream staining procedures for light and electron microscopy is included. Development of computer vision applications for automated recognition and structural analysis of polytene chromosomes are discussed. Prospective and collaborative studies are described.U of I OnlyRestricted to the U of I community idenfinitely during batch ingest of legacy ETD

    Theta and alpha band modulations reflect error-related adjustments in the auditory condensation task

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    Error commission leads to adaptive adjustments in a number of brain networks that subserve goal-directed behavior, resulting in either enhanced stimulus processing or increased motor threshold depending on the nature of errors committed. Here, we studied these adjustments by analyzing post-error modulations of alpha and theta band activity in the auditory version of the two-choice condensation task, which is highly demanding for sustained attention while involves no inhibition of prepotent responses. Errors were followed by increased frontal midline theta (FMT) activity, as well as by enhanced alpha band suppression in the parietal and the left central regions; parietal alpha suppression correlated with the task performance, left central alpha suppression correlated with the post-error slowing, and FMT increase correlated with both behavioral measures. On post-error correct trials, left-central alpha band suppression started earlier before the response, and the response was followed by weaker FMT activity, as well as by enhanced alpha band suppression distributed over the entire scalp. These findings indicate that several separate neuronal networks are involved in post-error adjustments, including the midfrontal performance monitoring network, the parietal attentional network, and the sensorimotor network. Supposedly, activity within these networks is rapidly modulated after errors, resulting in optimization of their functional state on the subsequent trials, with corresponding changes in behavioral measures
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