243 research outputs found

    No observational constraints from hypothetical collisions of hypothetical dark halo primordial black holes with galactic objects

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    It was suggested by several authors that hypothetical primordial black holes (PBHs) may contribute to the dark matter in our Galaxy. There are strong constraints based on the Hawking evaporation that practically exclude PBHs with masses m~1e15-1e16g and smaller as significant contributors to the Galactic dark matter. Similarly, PBHs with masses greater than about 1e26g are practically excluded by the gravitational lensing observation. The mass range between 10e16g<m<10e26g is unconstrained. In this paper, we examine possible observational signatures in the unexplored mass range, investigating hypothetical collisions of PBHs with main sequence stars, red giants, white dwarfs, and neutron stars in our Galaxy. This has previously been discussed as possibly leading to an observable photon eruption due to shock production during the encounter. We find that such collisions are either too rare to be observed (if the PBH masses are typically larger than about 1e20g), or produce too little power to be detected (if the masses are smaller than about 1e20g).Comment: Accepted for publication in The Astrophysical Journa

    The Bending Magnets for the Proton Transfer Line of CNGS

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    The project "CERN neutrinos to Gran Sasso (CNGS)", a collaboration between CERN and the INFN (Gran Sasso Laboratory) in Italy, will study neutrino oscillations in a long base-line experiment. High-energy protons will be extracted from the CERN SPS accelerator, transported through a 727 m long transfer line and focused onto a graphite target to produce a beam of pions and kaons and subsequently neutrinos. The transfer line requires a total of 78 dipole magnets. They were produced in the framework of an in-kind contribution of Germany via DESY to the CNGS project. The normal conducting dipoles, built from laminated steel cores and copper coils, have a core length of 6.3 m, a 37 mm gap height and a nominal field range of 1.38 T - 1.91 T at a maximum current of 4950 A. The magnet design was a collaboration between CERN and BINP. The half-core production was subcontracted to EFREMOV Institute; the coil fabrication, magnet assembly and the field measurements were concluded at BINP in June 2004. The main design issues and results of the acceptance tests, including mechanical, electrical and magnetic field measurements, are discussed

    Polariton propagation in weak confinement quantum wells

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    Exciton-polariton propagation in a quantum well, under centre-of-mass quantization, is computed by a variational self-consistent microscopic theory. The Wannier exciton envelope functions basis set is given by the simple analytical model of ref. [1], based on pure states of the centre-of-mass wave vector, free from fitting parameters and "ad hoc" (the so called additional boundary conditions-ABCs) assumptions. In the present paper, the former analytical model is implemented in order to reproduce the centre-of-mass quantization in a large range of quantum well thicknesses (5a_B < L < inf.). The role of the dynamical transition layer at the well/barrier interfaces is discussed at variance of the classical Pekar's dead-layer and ABCs. The Wannier exciton eigenstates are computed, and compared with various theoretical models with different degrees of accuracy. Exciton-polariton transmission spectra in large quantum wells (L>> a_B) are computed and compared with experimental results of Schneider et al.\cite{Schneider} in high quality GaAs samples. The sound agreement between theory and experiment allows to unambiguously assign the exciton-polariton dips of the transmission spectrum to the pure states of the Wannier exciton center-of-mass quantization.Comment: 15 pages, 15 figures; will appear in Phys.Rev.

    Peak Stir Zone Temperatures during Friction Stir Processing

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    The stir zone (SZ) temperature cycle was measured during the friction stir processing (FSP) of NiAl bronze plates. The FSP was conducted using a tool design with a smooth concave shoulder and a 12.7-mm step-spiral pin. Temperature sensing was accomplished using sheathed thermocouples embedded in the tool path within the plates, while simultaneous optical pyrometry measurements of surface temperatures were also obtained. Peak SZ temperatures were 990 ⁰Cto 1015 ⁰C (0.90 to 0.97 TMelt) and were not affected by preheating to 400⁰C, although the dwell time above 900 ⁰C was increased by the preheating. Thermocouple data suggested little variation in peak temperature across the SZ, although thermocouples initially located on the advancing sides and at the centerlines of the tool traverses were displaced to the retreating sides, precluding direct assessment of the temperature variation across the SZ. Microstructure-based estimates of local peak SZ temperatures have been made on these and on other similarly processed materials. Altogether, the peak-temperature determinations from these different measurement techniques are in close agreement

    ΠŸΡ€Π΅Π΄ΠΈΠΊΡ‚ΠΎΡ€Ρ‹ ΠΎΡ‚ΠΌΠ΅Π½Ρ‹ Π³Π΅Π½Π½ΠΎ-ΠΈΠ½ΠΆΠ΅Π½Π΅Ρ€Π½Ρ‹Ρ… биологичСских ΠΏΡ€Π΅ΠΏΠ°Ρ€Π°Ρ‚ΠΎΠ² Π²Π²ΠΈΠ΄Ρƒ развития Π½Π΅ΠΆΠ΅Π»Π°Ρ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… явлСний Ρƒ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ² с Ρ€Π΅Π²ΠΌΠ°Ρ‚ΠΎΠΈΠ΄Π½Ρ‹ΠΌ Π°Ρ€Ρ‚Ρ€ΠΈΡ‚ΠΎΠΌ

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    Currently, a large number of highly effective biologic disease modifying antirheumatic drugs (bDMARDs) and targeted synthetic DMARDs (tsDMARDs) are used for the treatment of rheumatoid arthritis (RA). However, in addition to effectiveness, it is necessary to evaluate the risk of adverse events (AEs) when using them.Objective: to determine the predictors of bDMARDs and tsDMARDs discontinuation due to AEs in patients with RA.Patients and methods. The study included 661 patients with RA who took bDMARDs and tsDMARDs. The search for predictors of targeted therapy discontinuation due to AEs was carried out in two stages. At the first stage, using the Kaplan-Meier method, we selected indicators that showed the greatest significant single-factor relationship with the duration of retention on therapy. At the second stage, significant independent indicators were obtained by iterative selection of variables within the multivariate proportional risk model according to Cox.Results and discussion. The presence of rheumatoid nodules (p&lt;0.001), high doses of glucocorticoids (GC; p&lt;0.001), low doses of methotrexate (MT; p=0.009) are significant independent factors for increasing the risk of drugs discontinuation due to the development of AEs. The type of bDMARDs/tsDMARD used also significantly correlated with the risk of discontinuation of therapy due to AEs. A relatively high risk of treatment discontinuation was observed with infliximab (IFN) and certolizumab pegol (CZP). Cancellation of IFN was associated with the occurrence of infusion reactions and infectious complications, and CZP was associated with infectious complications.Conclusion. An increase in the dose of MT and decrease in the use of GCs can help prevent the development of AEs leading to the abolition of biologics and tsDMARDs. Significant differences were found between bDMARDs in terms of the risk of their cancellation due to AEs.Π’ настоящСС врСмя для лСчСния Ρ€Π΅Π²ΠΌΠ°Ρ‚ΠΎΠΈΠ΄Π½ΠΎΠ³ΠΎ Π°Ρ€Ρ‚Ρ€ΠΈΡ‚Π° (РА) ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΡƒΠ΅Ρ‚ΡΡ большоС число Π³Π΅Π½Π½ΠΎ-ΠΈΠ½ΠΆΠ΅Π½Π΅Ρ€Π½Ρ‹Ρ… биологичСских (Π“Π˜Π‘ΠŸ) ΠΈ Ρ‚Π°Ρ€Π³Π΅Ρ‚Π½Ρ‹Ρ… синтСтичСских базисных ΠΏΡ€ΠΎΡ‚ΠΈΠ²ΠΎΠ²ΠΎΡΠΏΠ°Π»ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… ΠΏΡ€Π΅ΠΏΠ°Ρ€Π°Ρ‚ΠΎΠ² (Ρ‚ΡΠ‘ΠŸΠ’ΠŸ), ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ ΠΎΠ±Π»Π°Π΄Π°ΡŽΡ‚ высокой ΡΡ„Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒΡŽ. Однако, ΠΏΠΎΠΌΠΈΠΌΠΎ эффСктивности, Π½Π΅ΠΎΠ±Ρ…ΠΎΠ΄ΠΈΠΌΠΎ ΠΎΡ†Π΅Π½ΠΈΠ²Π°Ρ‚ΡŒ риск возникновСния Π½Π΅ΠΆΠ΅Π»Π°Ρ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… явлСний (НЯ) ΠΏΡ€ΠΈ ΠΈΡ… использовании.ЦСль исслСдования β€” ΠΎΠΏΡ€Π΅Π΄Π΅Π»ΠΈΡ‚ΡŒ ΠΏΡ€Π΅Π΄ΠΈΠΊΡ‚ΠΎΡ€Ρ‹ ΠΎΡ‚ΠΌΠ΅Π½Ρ‹ Π“Π˜Π‘ΠŸ ΠΈ Ρ‚ΡΠ‘ΠŸΠ’ΠŸ ΠΈΠ·-Π·Π° НЯ Ρƒ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ² с РА.ΠŸΠ°Ρ†ΠΈΠ΅Π½Ρ‚Ρ‹ ΠΈ ΠΌΠ΅Ρ‚ΠΎΠ΄Ρ‹. Π’ исслСдованиС Π²ΠΊΠ»ΡŽΡ‡Π΅Π½ 661 ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ с РА, ΠΏΡ€ΠΈΠ½ΠΈΠΌΠ°Π²ΡˆΠΈΠΉ Π“Π˜Π‘ΠŸ ΠΈ Ρ‚ΡΠ‘ΠŸΠ’ΠŸ. Поиск ΠΏΡ€Π΅Π΄ΠΈΠΊΡ‚ΠΎΡ€ΠΎΠ² ΠΎΡ‚ΠΌΠ΅Π½Ρ‹ Ρ‚Π°Ρ€Π³Π΅Ρ‚Π½ΠΎΠΉ Ρ‚Π΅Ρ€Π°ΠΏΠΈΠΈ Π²Π²ΠΈΠ΄Ρƒ НЯ проводился Π² Π΄Π²Π° этапа. На ΠΏΠ΅Ρ€Π²ΠΎΠΌ этапС с ΠΏΠΎΠΌΠΎΡ‰ΡŒΡŽ ΠΌΠ΅Ρ‚ΠΎΠ΄Π° ΠšΠ°ΠΏΠ»Π°Π½Π°β€”ΠœΠ°ΠΉΠ΅Ρ€Π° Π±Ρ‹Π»ΠΈ ΠΎΡ‚ΠΎΠ±Ρ€Π°Π½Ρ‹ ΠΏΠΎΠΊΠ°Π·Π°Ρ‚Π΅Π»ΠΈ, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ дСмонстрировали Π½Π°ΠΈΠ±ΠΎΠ»ΡŒΡˆΡƒΡŽ Π·Π½Π°Ρ‡ΠΈΠΌΡƒΡŽ ΠΎΠ΄Π½ΠΎΡ„Π°ΠΊΡ‚ΠΎΡ€Π½ΡƒΡŽ связь с Π΄Π»ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΡΡ‚ΡŒΡŽ удСрТания Π½Π° Ρ‚Π΅Ρ€Π°ΠΏΠΈΠΈ. На Π²Ρ‚ΠΎΡ€ΠΎΠΌ этапС Π·Π½Π°Ρ‡ΠΈΠΌΡ‹Π΅ нСзависимыС ΠΏΠΎΠΊΠ°Π·Π°Ρ‚Π΅Π»ΠΈ Π±Ρ‹Π»ΠΈ ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Ρ‹ ΠΏΡƒΡ‚Π΅ΠΌ пошагового ΠΎΡ‚Π±ΠΎΡ€Π° ΠΏΠ΅Ρ€Π΅ΠΌΠ΅Π½Π½Ρ‹Ρ… Π² Ρ€Π°ΠΌΠΊΠ°Ρ… ΠΌΠ½ΠΎΠ³ΠΎΡ„Π°ΠΊΡ‚ΠΎΡ€Π½ΠΎΠΉ ΠΌΠΎΠ΄Π΅Π»ΠΈ ΠΏΡ€ΠΎΠΏΠΎΡ€Ρ†ΠΈΠΎΠ½Π°Π»ΡŒΠ½ΠΎΠ³ΠΎ риска ΠΏΠΎ ΠšΠΎΠΊΡΡƒ.Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ ΠΈ обсуТдСниС. НаличиС Ρ€Π΅Π²ΠΌΠ°Ρ‚ΠΎΠΈΠ΄Π½Ρ‹Ρ… ΡƒΠ·Π΅Π»ΠΊΠΎΠ² (p&lt;0,001), высокиС Π΄ΠΎΠ·Ρ‹ Π³Π»ΡŽΠΊΠΎΠΊΠΎΡ€Ρ‚ΠΈΠΊΠΎΠΈΠ΄ΠΎΠ² (Π“Πš; p&lt;0,001), Π½ΠΈΠ·ΠΊΠΈΠ΅ Π΄ΠΎΠ·Ρ‹ мСтотрСксата (МВ; p=0,009) ΡΠ²Π»ΡΡŽΡ‚ΡΡ Π·Π½Π°Ρ‡ΠΈΠΌΡ‹ΠΌΠΈ нСзависимыми Ρ„Π°ΠΊΡ‚ΠΎΡ€Π°ΠΌΠΈ увСличСния риска ΠΎΡ‚ΠΌΠ΅Π½Ρ‹ ΠΏΡ€Π΅ΠΏΠ°Ρ€Π°Ρ‚ΠΎΠ² ΠΈΠ·-Π·Π° развития НЯ. Π˜ΡΠΏΠΎΠ»ΡŒΠ·ΡƒΠ΅ΠΌΡ‹ΠΉ Π“Π˜Π‘ΠŸ/Ρ‚ΡΠ‘ΠŸΠ’ΠŸ Ρ‚Π°ΠΊΠΆΠ΅ Π·Π½Π°Ρ‡ΠΈΠΌΠΎ ΠΊΠΎΡ€Ρ€Π΅Π»ΠΈΡ€ΠΎΠ²Π°Π» с риском ΠΎΡ‚ΠΌΠ΅Π½Ρ‹ Ρ‚Π΅Ρ€Π°ΠΏΠΈΠΈ ΠΈΠ·-Π·Π° НЯ. ΠžΡ‚Π½ΠΎΡΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ высокий риск прСкращСния лСчСния Π±Ρ‹Π» ΠΎΡ‚ΠΌΠ΅Ρ‡Π΅Π½ Ρƒ инфликсимаба (ИНЀ) ΠΈ Ρ†Π΅Ρ€Ρ‚ΠΎΠ»ΠΈΠ·ΡƒΠΌΠ°Π±Π° пэгола (Π¦Π—ΠŸ). ΠžΡ‚ΠΌΠ΅Π½Π° ИНЀ Π±Ρ‹Π»Π° связана с Π²ΠΎΠ·Π½ΠΈΠΊΠ½ΠΎΠ²Π΅Π½ΠΈΠ΅ΠΌ ΠΈΠ½Ρ„ΡƒΠ·ΠΈΠΎΠ½Π½Ρ‹Ρ… Ρ€Π΅Π°ΠΊΡ†ΠΈΠΉ ΠΈ ΠΈΠ½Ρ„Π΅ΠΊΡ†ΠΈΠΎΠ½Π½Ρ‹Ρ… ослоТнСний, Π° Π¦Π—ΠŸ β€” с ΠΈΠ½Ρ„Π΅ΠΊΡ†ΠΈΠΎΠ½Π½Ρ‹ΠΌΠΈ ослоТнСниями.Π—Π°ΠΊΠ»ΡŽΡ‡Π΅Π½ΠΈΠ΅. Π£Π²Π΅Π»ΠΈΡ‡Π΅Π½ΠΈΠ΅ Π΄ΠΎΠ·Ρ‹ МВ, ΡƒΠΌΠ΅Π½ΡŒΡˆΠ΅Π½ΠΈΠ΅ использования Π“ΠšΠΌΠΎΠ³ΡƒΡ‚ ΡΠΏΠΎΡΠΎΠ±ΡΡ‚Π²ΠΎΠ²Π°Ρ‚ΡŒ ΠΏΡ€Π΅Π΄ΠΎΡ‚Π²Ρ€Π°Ρ‰Π΅Π½ΠΈΡŽ развития НЯ, приводящих ΠΊ ΠΎΡ‚ΠΌΠ΅Π½Π΅ Π“Π˜Π‘ΠŸ ΠΈ Ρ‚ΡΠ‘ΠŸΠ’ΠŸ. ВыявлСны сущСствСнныС различия ΠΌΠ΅ΠΆΠ΄Ρƒ Π“Π˜Π‘ΠŸ Π² ΠΎΡ‚Π½ΠΎΡˆΠ΅Π½ΠΈΠΈ риска ΠΈΡ… ΠΎΡ‚ΠΌΠ΅Π½Ρ‹ вслСдствиС НЯ
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