133 research outputs found

    Magnetocrystalline anisotropic effect in GdCo1βˆ’x_{1-x}Fex_xAsO (x=0,0.05x = 0, 0.05)

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    From a systematic study of the electrical resistivity ρ(T,H)\rho(T,H), magnetic susceptibility Ο‡(T,H)\chi(T,H), isothermal magnetization M(H)M(H) and the specific heat C(T,H)C(T,H), a temperature-magnetic field (TT-HH) phase diagram has been established for GdCo1βˆ’x_{1-x}Fex_xAsO (x=0x = 0 and 0.050.05) polycrystalline compounds. GdCoAsO undergoes two long-range magnetic transitions: ferromagnetic (FM) transition of Co 3d3d electrons (TCCoT_\textup{C}^\textup{Co}) and antiferromagnetic (AFM) transition of Gd 4f4f electrons (TNGdT_\textup{N}^\textup{Gd}). For the Fe-doped sample (x=0.05x=0.05), an extra magnetic reorientation transition takes place below TNGdT_\textup{N}^\textup{Gd}, which is likely associated with Co moments. The two magnetic species of Gd and Co are coupled antiferromagnetically to give rise to ferrimagnetic (FIM) behavior in the magnetic susceptibility. Upon decreasing the temperature (T<TCCoT < T_\textup{C}^\textup{Co}), the magnetocrystalline anisotropy breaks up the FM order of Co by aligning the moments with the local easy axes of the various grains, leading to a spin reorientation transition at TRCoT_\textup{R}^\textup{Co}. By applying a magnetic field, TRCoT_\textup{R}^\textup{Co} monotonically decreases to lower temperatures, while the TNGdT_\textup{N}^\textup{Gd} is relatively robust against the external field. On the other hand, the applied magnetic field pulls the magnetization of grains from the local easy direction to the field direction via a first-order reorientation transition, with the transition field (HMH_\textup{M}) increasing upon cooling the temperature.Comment: accepted by physical Review B 6 figures and 7 page

    Observation of inhibited spontaneous emission and stimulated emission of rhodamine 6G in polymer replica of synthetic opal

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    This article may be downloaded for personal use only. Any other use requires prior permission of the author and AIP Publishing. This article appeared in K. Yoshino, S. B. Lee,b) S. Tatsuhara, Y. Kawagishi, and M. Ozaki, and A. A. Zakhidov, Appl. Phys. Lett. 73, 3506 (1998) and may be found at https://doi.org/10.1063/1.122819

    Nonlocal electrodynamics of two-dimensional wire mesh photonic crystals

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    We calculate analytically the spectra of plasma waves and electromagnetic waves (EMW) in metallic photonic crystal consisting of the parallel thin infinite metallic cylinders embedded in the dielectric media. The axes of metallic cylinders form a regular square lattice in a plane perpendicular to them. The metal inside the cylinders is assumed to be in the high frequency regime ωτ>>1\omega \tau >> 1, where Ο„\tau is the relaxation time. The proposed analytical theory is based upon small parameters f<<1f << 1, where ff is the volume fraction of the metal, and kR<<1kR << 1, where kk is the wave vector and RR is the radius of the cylinder. It is shown that there are five different branches of the EMW that cover all frequency range under consideration except one very small omnidirectional gap in the vicinity of the frequency of the surface plasmon. However, at some directions of propagation and polarizations the gap may be much larger. The reflection and refraction of the EMW is also considered. The general theory of refraction is proposed which is complicated by the spatial dispersion of the dielectric constant, and one particular geometry of the incident EMW is considered.Comment: 14 pages, 8 figure

    Braggoriton--Excitation in Photonic Crystal Infiltrated with Polarizable Medium

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    Light propagation in a photonic crystal infiltrated with polarizable molecules is considered. We demonstrate that the interplay between the spatial dispersion caused by Bragg diffraction and polaritonic frequency dispersion gives rise to novel propagating excitations, or braggoritons, with intragap frequencies. We derive the braggoriton dispersion relation and show that it is governed by two parameters, namely, the strength of light-matter interaction and detuning between the Bragg frequency and that of the infiltrated molecules. We also study defect-induced states when the photonic band gap is divided into two subgaps by the braggoritonic branches and find that each defect creates two intragap localized states inside each subgap.Comment: LaTeX, 8 pages, 5 figure

    Silver nanowires on carbon nanotube aerogel sheets for flexible, transparent electrodes

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    Flexible, free-standing transparent conducting electrodes (TCEs) with simultaneously tunable transmittances up to 98% and sheet resistances down to 11 Ω/sq were prepared by a facile spray-coating method of silver nanowires (AgNWs) onto dry-spun multiwall carbon nanotube (MWNT) aerogels. Counterintuitively, the transmittance of the hybrid electrodes can be increased as the mass density of AgNWs within the MWNT aerogels increases, however, the final achievable transmittance depends on the initial transparency of the MWNT aerogels. Simultaneously, a strong decrease in sheet resistance is obtained when AgNWs form a percolated network along the MWNT aerogel. Additionally, anisotropic reduction in sheet resistance and polarized transmittance of AgNW/MWNT aerogels is achieved with this method. The final AgNW/MWNT hybrid TCEs transmittance and sheet resistance can be fine-tuned by spray-coating mechanisms or by choosing initial MWNT aerogel density. Thus, a wide range of AgNW/MWNT hybrid TCEs with optimized optoelectronic properties can be achieved depending of the requirements needed. Finally, the free-standing AgNW/MWNT hybrid TCEs can be laminated onto a wide range of substrates without the need of a bonding aid

    Риски хирургичСского лСчСния Π³Π»Π°ΡƒΠΊΠΎΠΌΡ‹ Π½Π° СдинствСнном видящСм Π³Π»Π°Π·Ρƒ с далСкозашСдшСй стадиСй заболСвания

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    This review summarizes the results of surgical treatment of far-advanced stage glaucoma in the only seeing eye. A literature search performed in the PubMed search engine and aimed at finding publications reporting the clinical outcomes of treatment in patients with glaucoma in the only seeing eye did yield sufficient data related to the topic. A comprehensive analysis of the available data was performed with an emphasis on the choice of treatment tactics and postoperative results at various times following a surgery. Several studies allowed to perform a comparison of the clinical advantages and cost-effectiveness of medical treatment versus surgery for advanced glaucoma, as well as to assess potential risks and adverse outcomes such as glaucoma progression, postoperative scarring, hypotension and other complications. The results presented in this review suggest that common success criteria can provide uniformity in academic studies, but in daily clinical practice each glaucoma specialist must make a patient-specific decision in favor of either of these methods of treatment in order to guarantee an optimal result, both for the doctor and, of course, for the patient.ЦСль ΠΎΠ±Π·ΠΎΡ€Π° β€” ΠΎΠ±ΠΎΠ±Ρ‰ΠΈΡ‚ΡŒ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹, ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Π΅ послС ΠΏΡ€ΠΎΠ²Π΅Π΄Π΅Π½Π½ΠΎΠ³ΠΎ хирургичСского лСчСния далСкозашСдшСй стадии Π³Π»Π°ΡƒΠΊΠΎΠΌΡ‹ Π½Π° СдинствСнно видящСм Π³Π»Π°Π·Ρƒ. Поиск Π»ΠΈΡ‚Π΅Ρ€Π°Ρ‚ΡƒΡ€Ρ‹, Π²Ρ‹ΠΏΠΎΠ»Π½Π΅Π½Π½Ρ‹ΠΉ Π² поисковой систСмС PubMed ΠΈ Π½Π°ΠΏΡ€Π°Π²Π»Π΅Π½Π½Ρ‹ΠΉ Π½Π° ΠΎΠ±Π½Π°Ρ€ΡƒΠΆΠ΅Π½ΠΈΠ΅ ΠΏΡƒΠ±Π»ΠΈΠΊΠ°Ρ†ΠΈΠΉ, ΡΠΎΠΎΠ±Ρ‰Π°ΡŽΡ‰ΠΈΡ… ΠΎ клиничСских Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Π°Ρ… ΠΏΡ€ΠΎΠ²Π΅Π΄Π΅Π½Π½ΠΎΠ³ΠΎ лСчСния Ρƒ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ² с Π³Π»Π°ΡƒΠΊΠΎΠΌΠΎΠΉ Π½Π° СдинствСнно видящСм Π³Π»Π°Π·Ρƒ, Π½Π΅ ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΠ» Π½Π°ΠΌ Π½Π°ΠΉΡ‚ΠΈ достаточного объСма Ρ‚Π°ΠΊΠΎΠ³ΠΎ Ρ€ΠΎΠ΄Π° исслСдований. ΠŸΡ€ΠΎΠ²Π΅Π΄Π΅Π½ всСсторонний Π°Π½Π°Π»ΠΈΠ· ΠΈΠΌΠ΅ΡŽΡ‰ΠΈΡ…ΡΡ Π΄Π°Π½Π½Ρ‹Ρ… с Π°ΠΊΡ†Π΅Π½Ρ‚ΠΎΠΌ Π½Π° Π²Ρ‹Π±ΠΎΡ€ Ρ‚Π°ΠΊΡ‚ΠΈΠΊΠΈ лСчСния ΠΈ послСопСрационныС Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ Π² Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Π΅ сроки послС ΠΎΠΏΠ΅Ρ€Π°Ρ†ΠΈΠΈ. НСкоторыС исслСдования ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΠ»ΠΈ ΡΡ€Π°Π²Π½ΠΈΡ‚ΡŒ ΠΊΠ»ΠΈΠ½ΠΈΡ‡Π΅ΡΠΊΡƒΡŽ ΠΈ ΡΠΊΠΎΠ½ΠΎΠΌΠΈΡ‡Π΅ΡΠΊΡƒΡŽ ΡΡ„Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒ ΠΌΠ΅Π΄ΠΈΠΊΠ°ΠΌΠ΅Π½Ρ‚ΠΎΠ·Π½ΠΎΠ³ΠΎ лСчСния ΠΏΠΎ ΡΡ€Π°Π²Π½Π΅Π½ΠΈΡŽ с хирургичСским Π»Π΅Ρ‡Π΅Π½ΠΈΠ΅ΠΌ далСкозашСдшСй стадии Π³Π»Π°ΡƒΠΊΠΎΠΌΡ‹, Π° Ρ‚Π°ΠΊΠΆΠ΅ ΠΎΡ†Π΅Π½ΠΈΡ‚ΡŒ вСроятныС риски ΠΈ нСблагоприятныС исходы, Ρ‚Π°ΠΊΠΈΠ΅ ΠΊΠ°ΠΊ прогрСссированиС Π³Π»Π°ΡƒΠΊΠΎΠΌΡ‹, послСопСрационноС Ρ€ΡƒΠ±Ρ†Π΅Π²Π°Π½ΠΈΠ΅, Π³ΠΈΠΏΠΎΡ‚ΠΎΠ½ΠΈΡŽ ΠΈ Π΄Ρ€ΡƒΠ³ΠΈΠ΅ ослоТнСния. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹, прСдставлСнныС Π² ΠΎΠ±Π·ΠΎΡ€Π΅, ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡŽΡ‚ ΡΠ΄Π΅Π»Π°Ρ‚ΡŒ Π²Ρ‹Π²ΠΎΠ΄, Ρ‡Ρ‚ΠΎ ΠΎΠ±Ρ‰ΠΈΠ΅ ΠΊΡ€ΠΈΡ‚Π΅Ρ€ΠΈΠΈ успСха ΠΌΠΎΠ³ΡƒΡ‚ ΠΎΠ±Π΅ΡΠΏΠ΅Ρ‡ΠΈΡ‚ΡŒ ΠΎΠ΄Π½ΠΎΡ€ΠΎΠ΄Π½ΠΎΡΡ‚ΡŒ Π² акадСмичСских исслСдованиях, Π½ΠΎ Π² повсСднСвной клиничСской ΠΏΡ€Π°ΠΊΡ‚ΠΈΠΊΠ΅ ΠΊΠ°ΠΆΠ΄Ρ‹ΠΉ Π³Π»Π°ΡƒΠΊΠΎΠΌΠ°Ρ‚ΠΎΠ»ΠΎΠ³ Π΄ΠΎΠ»ΠΆΠ΅Π½ ΠΈΠ½Π΄ΠΈΠ²ΠΈΠ΄ΡƒΠ°Π»ΡŒΠ½ΠΎ ΠΏΡ€ΠΈΠ½ΠΈΠΌΠ°Ρ‚ΡŒ Ρ€Π΅ΡˆΠ΅Π½ΠΈΠ΅ Π² ΠΏΠΎΠ»ΡŒΠ·Ρƒ Ρ‚ΠΎΠ³ΠΎ ΠΈΠ»ΠΈ ΠΈΠ½ΠΎΠ³ΠΎ ΠΌΠ΅Ρ‚ΠΎΠ΄Π° лСчСния, Ρ‡Ρ‚ΠΎΠ±Ρ‹ Π³Π°Ρ€Π°Π½Ρ‚ΠΈΡ€ΠΎΠ²Π°Ρ‚ΡŒ ΠΎΠΏΡ‚ΠΈΠΌΠ°Π»ΡŒΠ½Ρ‹ΠΉ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚, ΠΊΠ°ΠΊ для Π²Ρ€Π°Ρ‡Π°, Ρ‚Π°ΠΊ ΠΈ, СстСствСнно, для ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚Π°
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