243 research outputs found
No observational constraints from hypothetical collisions of hypothetical dark halo primordial black holes with galactic objects
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
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
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
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 β°Cto 1015 β°C (0.90 to 0.97 TMelt) and were not affected by preheating to 400β°C, although the dwell time above 900 β°C 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
ΠΡΠ΅Π΄ΠΈΠΊΡΠΎΡΡ ΠΎΡΠΌΠ΅Π½Ρ Π³Π΅Π½Π½ΠΎ-ΠΈΠ½ΠΆΠ΅Π½Π΅ΡΠ½ΡΡ Π±ΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ ΠΏΡΠ΅ΠΏΠ°ΡΠ°ΡΠΎΠ² Π²Π²ΠΈΠ΄Ρ ΡΠ°Π·Π²ΠΈΡΠΈΡ Π½Π΅ΠΆΠ΅Π»Π°ΡΠ΅Π»ΡΠ½ΡΡ ΡΠ²Π»Π΅Π½ΠΈΠΉ Ρ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Ρ ΡΠ΅Π²ΠΌΠ°ΡΠΎΠΈΠ΄Π½ΡΠΌ Π°ΡΡΡΠΈΡΠΎΠΌ
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<0.001), high doses of glucocorticoids (GC; p<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 Π½Π°ΡΡΠΎΡΡΠ΅Π΅ Π²ΡΠ΅ΠΌΡ Π΄Π»Ρ Π»Π΅ΡΠ΅Π½ΠΈΡ ΡΠ΅Π²ΠΌΠ°ΡΠΎΠΈΠ΄Π½ΠΎΠ³ΠΎ Π°ΡΡΡΠΈΡΠ° (Π Π) ΠΈΡΠΏΠΎΠ»ΡΠ·ΡΠ΅ΡΡΡ Π±ΠΎΠ»ΡΡΠΎΠ΅ ΡΠΈΡΠ»ΠΎ Π³Π΅Π½Π½ΠΎ-ΠΈΠ½ΠΆΠ΅Π½Π΅ΡΠ½ΡΡ
Π±ΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
(ΠΠΠΠ) ΠΈ ΡΠ°ΡΠ³Π΅ΡΠ½ΡΡ
ΡΠΈΠ½ΡΠ΅ΡΠΈΡΠ΅ΡΠΊΠΈΡ
Π±Π°Π·ΠΈΡΠ½ΡΡ
ΠΏΡΠΎΡΠΈΠ²ΠΎΠ²ΠΎΡΠΏΠ°Π»ΠΈΡΠ΅Π»ΡΠ½ΡΡ
ΠΏΡΠ΅ΠΏΠ°ΡΠ°ΡΠΎΠ² (ΡΡΠΠΠΠ), ΠΊΠΎΡΠΎΡΡΠ΅ ΠΎΠ±Π»Π°Π΄Π°ΡΡ Π²ΡΡΠΎΠΊΠΎΠΉ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΡΡ. ΠΠ΄Π½Π°ΠΊΠΎ, ΠΏΠΎΠΌΠΈΠΌΠΎ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ, Π½Π΅ΠΎΠ±Ρ
ΠΎΠ΄ΠΈΠΌΠΎ ΠΎΡΠ΅Π½ΠΈΠ²Π°ΡΡ ΡΠΈΡΠΊ Π²ΠΎΠ·Π½ΠΈΠΊΠ½ΠΎΠ²Π΅Π½ΠΈΡ Π½Π΅ΠΆΠ΅Π»Π°ΡΠ΅Π»ΡΠ½ΡΡ
ΡΠ²Π»Π΅Π½ΠΈΠΉ (ΠΠ―) ΠΏΡΠΈ ΠΈΡ
ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠΈ.Π¦Π΅Π»Ρ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ β ΠΎΠΏΡΠ΅Π΄Π΅Π»ΠΈΡΡ ΠΏΡΠ΅Π΄ΠΈΠΊΡΠΎΡΡ ΠΎΡΠΌΠ΅Π½Ρ ΠΠΠΠ ΠΈ ΡΡΠΠΠΠ ΠΈΠ·-Π·Π° ΠΠ― Ρ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Ρ Π Π.ΠΠ°ΡΠΈΠ΅Π½ΡΡ ΠΈ ΠΌΠ΅ΡΠΎΠ΄Ρ. Π ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ Π²ΠΊΠ»ΡΡΠ΅Π½ 661 ΠΏΠ°ΡΠΈΠ΅Π½Ρ Ρ Π Π, ΠΏΡΠΈΠ½ΠΈΠΌΠ°Π²ΡΠΈΠΉ ΠΠΠΠ ΠΈ ΡΡΠΠΠΠ. ΠΠΎΠΈΡΠΊ ΠΏΡΠ΅Π΄ΠΈΠΊΡΠΎΡΠΎΠ² ΠΎΡΠΌΠ΅Π½Ρ ΡΠ°ΡΠ³Π΅ΡΠ½ΠΎΠΉ ΡΠ΅ΡΠ°ΠΏΠΈΠΈ Π²Π²ΠΈΠ΄Ρ ΠΠ― ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»ΡΡ Π² Π΄Π²Π° ΡΡΠ°ΠΏΠ°. ΠΠ° ΠΏΠ΅ΡΠ²ΠΎΠΌ ΡΡΠ°ΠΏΠ΅ Ρ ΠΏΠΎΠΌΠΎΡΡΡ ΠΌΠ΅ΡΠΎΠ΄Π° ΠΠ°ΠΏΠ»Π°Π½Π°βΠΠ°ΠΉΠ΅ΡΠ° Π±ΡΠ»ΠΈ ΠΎΡΠΎΠ±ΡΠ°Π½Ρ ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»ΠΈ, ΠΊΠΎΡΠΎΡΡΠ΅ Π΄Π΅ΠΌΠΎΠ½ΡΡΡΠΈΡΠΎΠ²Π°Π»ΠΈ Π½Π°ΠΈΠ±ΠΎΠ»ΡΡΡΡ Π·Π½Π°ΡΠΈΠΌΡΡ ΠΎΠ΄Π½ΠΎΡΠ°ΠΊΡΠΎΡΠ½ΡΡ ΡΠ²ΡΠ·Ρ Ρ Π΄Π»ΠΈΡΠ΅Π»ΡΠ½ΠΎΡΡΡΡ ΡΠ΄Π΅ΡΠΆΠ°Π½ΠΈΡ Π½Π° ΡΠ΅ΡΠ°ΠΏΠΈΠΈ. ΠΠ° Π²ΡΠΎΡΠΎΠΌ ΡΡΠ°ΠΏΠ΅ Π·Π½Π°ΡΠΈΠΌΡΠ΅ Π½Π΅Π·Π°Π²ΠΈΡΠΈΠΌΡΠ΅ ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»ΠΈ Π±ΡΠ»ΠΈ ΠΏΠΎΠ»ΡΡΠ΅Π½Ρ ΠΏΡΡΠ΅ΠΌ ΠΏΠΎΡΠ°Π³ΠΎΠ²ΠΎΠ³ΠΎ ΠΎΡΠ±ΠΎΡΠ° ΠΏΠ΅ΡΠ΅ΠΌΠ΅Π½Π½ΡΡ
Π² ΡΠ°ΠΌΠΊΠ°Ρ
ΠΌΠ½ΠΎΠ³ΠΎΡΠ°ΠΊΡΠΎΡΠ½ΠΎΠΉ ΠΌΠΎΠ΄Π΅Π»ΠΈ ΠΏΡΠΎΠΏΠΎΡΡΠΈΠΎΠ½Π°Π»ΡΠ½ΠΎΠ³ΠΎ ΡΠΈΡΠΊΠ° ΠΏΠΎ ΠΠΎΠΊΡΡ.Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΈ ΠΎΠ±ΡΡΠΆΠ΄Π΅Π½ΠΈΠ΅. ΠΠ°Π»ΠΈΡΠΈΠ΅ ΡΠ΅Π²ΠΌΠ°ΡΠΎΠΈΠ΄Π½ΡΡ
ΡΠ·Π΅Π»ΠΊΠΎΠ² (p<0,001), Π²ΡΡΠΎΠΊΠΈΠ΅ Π΄ΠΎΠ·Ρ Π³Π»ΡΠΊΠΎΠΊΠΎΡΡΠΈΠΊΠΎΠΈΠ΄ΠΎΠ² (ΠΠ; p<0,001), Π½ΠΈΠ·ΠΊΠΈΠ΅ Π΄ΠΎΠ·Ρ ΠΌΠ΅ΡΠΎΡΡΠ΅ΠΊΡΠ°ΡΠ° (ΠΠ’; p=0,009) ΡΠ²Π»ΡΡΡΡΡ Π·Π½Π°ΡΠΈΠΌΡΠΌΠΈ Π½Π΅Π·Π°Π²ΠΈΡΠΈΠΌΡΠΌΠΈ ΡΠ°ΠΊΡΠΎΡΠ°ΠΌΠΈ ΡΠ²Π΅Π»ΠΈΡΠ΅Π½ΠΈΡ ΡΠΈΡΠΊΠ° ΠΎΡΠΌΠ΅Π½Ρ ΠΏΡΠ΅ΠΏΠ°ΡΠ°ΡΠΎΠ² ΠΈΠ·-Π·Π° ΡΠ°Π·Π²ΠΈΡΠΈΡ ΠΠ―. ΠΡΠΏΠΎΠ»ΡΠ·ΡΠ΅ΠΌΡΠΉ ΠΠΠΠ/ΡΡΠΠΠΠ ΡΠ°ΠΊΠΆΠ΅ Π·Π½Π°ΡΠΈΠΌΠΎ ΠΊΠΎΡΡΠ΅Π»ΠΈΡΠΎΠ²Π°Π» Ρ ΡΠΈΡΠΊΠΎΠΌ ΠΎΡΠΌΠ΅Π½Ρ ΡΠ΅ΡΠ°ΠΏΠΈΠΈ ΠΈΠ·-Π·Π° ΠΠ―. ΠΡΠ½ΠΎΡΠΈΡΠ΅Π»ΡΠ½ΠΎ Π²ΡΡΠΎΠΊΠΈΠΉ ΡΠΈΡΠΊ ΠΏΡΠ΅ΠΊΡΠ°ΡΠ΅Π½ΠΈΡ Π»Π΅ΡΠ΅Π½ΠΈΡ Π±ΡΠ» ΠΎΡΠΌΠ΅ΡΠ΅Π½ Ρ ΠΈΠ½ΡΠ»ΠΈΠΊΡΠΈΠΌΠ°Π±Π° (ΠΠΠ€) ΠΈ ΡΠ΅ΡΡΠΎΠ»ΠΈΠ·ΡΠΌΠ°Π±Π° ΠΏΡΠ³ΠΎΠ»Π° (Π¦ΠΠ). ΠΡΠΌΠ΅Π½Π° ΠΠΠ€ Π±ΡΠ»Π° ΡΠ²ΡΠ·Π°Π½Π° Ρ Π²ΠΎΠ·Π½ΠΈΠΊΠ½ΠΎΠ²Π΅Π½ΠΈΠ΅ΠΌ ΠΈΠ½ΡΡΠ·ΠΈΠΎΠ½Π½ΡΡ
ΡΠ΅Π°ΠΊΡΠΈΠΉ ΠΈ ΠΈΠ½ΡΠ΅ΠΊΡΠΈΠΎΠ½Π½ΡΡ
ΠΎΡΠ»ΠΎΠΆΠ½Π΅Π½ΠΈΠΉ, Π° Π¦ΠΠ β Ρ ΠΈΠ½ΡΠ΅ΠΊΡΠΈΠΎΠ½Π½ΡΠΌΠΈ ΠΎΡΠ»ΠΎΠΆΠ½Π΅Π½ΠΈΡΠΌΠΈ.ΠΠ°ΠΊΠ»ΡΡΠ΅Π½ΠΈΠ΅. Π£Π²Π΅Π»ΠΈΡΠ΅Π½ΠΈΠ΅ Π΄ΠΎΠ·Ρ ΠΠ’, ΡΠΌΠ΅Π½ΡΡΠ΅Π½ΠΈΠ΅ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ ΠΠΠΌΠΎΠ³ΡΡ ΡΠΏΠΎΡΠΎΠ±ΡΡΠ²ΠΎΠ²Π°ΡΡ ΠΏΡΠ΅Π΄ΠΎΡΠ²ΡΠ°ΡΠ΅Π½ΠΈΡ ΡΠ°Π·Π²ΠΈΡΠΈΡ ΠΠ―, ΠΏΡΠΈΠ²ΠΎΠ΄ΡΡΠΈΡ
ΠΊ ΠΎΡΠΌΠ΅Π½Π΅ ΠΠΠΠ ΠΈ ΡΡΠΠΠΠ. ΠΡΡΠ²Π»Π΅Π½Ρ ΡΡΡΠ΅ΡΡΠ²Π΅Π½Π½ΡΠ΅ ΡΠ°Π·Π»ΠΈΡΠΈΡ ΠΌΠ΅ΠΆΠ΄Ρ ΠΠΠΠ Π² ΠΎΡΠ½ΠΎΡΠ΅Π½ΠΈΠΈ ΡΠΈΡΠΊΠ° ΠΈΡ
ΠΎΡΠΌΠ΅Π½Ρ Π²ΡΠ»Π΅Π΄ΡΡΠ²ΠΈΠ΅ ΠΠ―
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