1,147 research outputs found

    Non-perturbative results for the spectrum of surface-disordered waveguides

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    We calculated the spectrum of normal scalar waves in a planar waveguide with absolutely soft randomly rough boundaries beyond the perturbation theories in the roughness heights and slopes, basing on the exact boundary scattering potential. The spectrum is proved to be a nearly real non-analytic function of the dispersion ζ2\zeta^2 of the roughness heights (with square-root singularity) as ζ2→0\zeta^2 \to 0. The opposite case of large boundary defects is summarized.Comment: REVTEX 3, OSA style, 9 pages, no figures. Submitted to Optics Letter

    A simple formula for the L-gap width of a face-centered-cubic photonic crystal

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    The width △L\triangle_L of the first Bragg's scattering peak in the (111) direction of a face-centered-cubic lattice of air spheres can be well approximated by a simple formula which only involves the volume averaged ϵ\epsilon and ϵ2\epsilon^2 over the lattice unit cell, ϵ\epsilon being the (position dependent) dielectric constant of the medium, and the effective dielectric constant ϵeff\epsilon_{eff} in the long-wavelength limit approximated by Maxwell-Garnett's formula. Apparently, our formula describes the asymptotic behaviour of the absolute gap width △L\triangle_L for high dielectric contrast δ\delta exactly. The standard deviation σ\sigma steadily decreases well below 1% as δ\delta increases. For example σ<0.1\sigma< 0.1% for the sphere filling fraction f=0.2f=0.2 and δ≥20\delta\geq 20. On the interval δ∈(1,100)\delta\in(1,100), our formula still approximates the absolute gap width △L\triangle_L (the relative gap width △Lr\triangle_L^r) with a reasonable precision, namely with a standard deviation 3% (4.2%) for low filling fractions up to 6.5% (8%) for the close-packed case. Differences between the case of air spheres in a dielectric and dielectric spheres in air are briefly discussed.Comment: 13 pages, 4 figs., RevTex, two references added. For more info see http://www.amolf.nl/external/wwwlab/atoms/theory/index.htm

    Photonic crystals of coated metallic spheres

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    It is shown that simple face-centered-cubic (fcc) structures of both metallic and coated metallic spheres are ideal candidates to achieve a tunable complete photonic bandgap (CPBG) for optical wavelengths using currently available experimental techniques. For coated microspheres with the coating width to plasma wavelength ratio lc/λp≤10l_c/\lambda_p \leq 10% and the coating and host refractive indices ncn_c and nhn_h, respectively, between 1 and 1.47, one can always find a sphere radius rsr_s such that the relative gap width gwg_w (gap width to the midgap frequency ratio) is larger than 5% and, in some cases, gwg_w can exceed 9%. Using different coatings and supporting liquids, the width and midgap frequency of a CPBG can be tuned considerably.Comment: 14 pages, plain latex, 3 ps figures, to appear in Europhys. Lett. For more info on this subject see http://www.amolf.nl/research/photonic_materials_theory/moroz/moroz.htm

    Photonic Band Gaps of Three-Dimensional Face-Centered Cubic Lattices

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    We show that the photonic analogue of the Korringa-Kohn-Rostocker method is a viable alternative to the plane-wave method to analyze the spectrum of electromagnetic waves in a three-dimensional periodic dielectric lattice. Firstly, in the case of an fcc lattice of homogeneous dielectric spheres, we reproduce the main features of the spectrum obtained by the plane wave method, namely that for a sufficiently high dielectric contrast a full gap opens in the spectrum between the eights and ninth bands if the dielectric constant ϵs\epsilon_s of spheres is lower than the dielectric constant ϵb\epsilon_b of the background medium. If ϵs>ϵb\epsilon_s> \epsilon_b, no gap is found in the spectrum. The maximal value of the relative band-gap width approaches 14% in the close-packed case and decreases monotonically as the filling fraction decreases. The lowest dielectric contrast ϵb/ϵs\epsilon_b/\epsilon_s for which a full gap opens in the spectrum is determined to be 8.13. Eventually, in the case of an fcc lattice of coated spheres, we demonstrate that a suitable coating can enhance gap widths by as much as 50%.Comment: 19 pages, 6 figs., plain latex - a section on coated spheres, two figures, and a few references adde

    Spectrophotometric experiment on the Verera-11 and Venera-12 descent vehicles: Some results of the analysis of the spectrum of the daytime sky of Venus

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    The spectra of the daytime sky of Venus were recorded on the Venera-11 and Venera-12 descent vehicles at various altitudes above the planet's surface, within the interval of 4500 to 12,000 Angstroms. The angular distribution of the brightness of the scattered radiation was recorded and the ratio of water and carbon dioxide were studied, with respect to the cloud cover boundaries

    Persistent currents in multicomponent Tomonaga-Luttinger liquid: application to mesoscopic semiconductor ring with spin-orbit interaction

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    We study persistent currents in semiconductor ballistic rings with spin-orbit Rashba interaction. We use as a working model the multicomponent Tomonaga-Luttinger liquid which arises due to the nonparabolic dispersion relations of electrons in the rings with rather strong spin-orbit coupling. This approach predicts some new characteristic features of persistent currents, which may be observed in experimental studies of semiconductor ballistic rings.Comment: 13 pages, 8 figure

    Comparison of the diagnostic efficiency of various noninvasive methods for diagnosing liver fibrosis in patients with chronic viral hepatitis C

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    Summary: the article presents the results of the examination of patients with chronic viral hepatitis C namely the study of the informativeness of instrumental (fibroelastography) and serological (the content of hyaluronic acid in serum) of markers of fibrosis by assessing their predictive value by ROC- analysis. The purpose of the study: to find out the possibility of non-invasive methods for diagnosing liver fibrosis in patients with chronic viral hepatitis C (CHC). Materials and methods 66 patients with CHC with the 1-st genotype of the virus were examined, which were at the dispensary observation and ambulatory treatment at DCC CCH №1 in Vinnitsa and in the clinical department of viral hepatitis at the Institute of Epidemiology and Infectious Diseases named after L.V. Gromashevsky NAMS of Ukraine. All patients received fibroelastography (FEG) with a METAVIR score. All patients with CHC and group of control determined the content of hyaluronic acid (GA) in blood serum (ELISA using the Hyaluronic Acid (Corgenix, Inc., USA)). Research results Sensitivity of determination of GA in blood serum of patients with CHC with degree of fibrosis of liver F0-F2 was 91.23%, and specificity - 90.46%. For the FEG method, respectively: 74.33% and 77.25%. In the group of patients with degree of fibrosis F3 sensitivity of the definition of GA in blood serum was 72.21%, and specificity - 74.71%. The corresponding qualitative characteristics for FEG were: 98.32% and 91.45% respectively. The sensitivity of the determination of the content of GA in serum of patients with CHC with the degree of liver fibrosis F4 was 88.23%, and the specificity was 92.12%. For these patients the sensitivity and specificity of determining the degree of fibrosis by the FEG method were 87.78% and 91.45% respectively. Conclusions High diagnostic efficiency of determination of the content of GA in serum was established for assessing the degree of liver fibrosis in patients with CSF (AUC = 0,720-0,917, p˂0,01). Relatively higher sensitivity and specificity of the diagnosis of liver fibrosis was observed in determining the content of GA in serum compared with the FEG method (AUC = 0.914 vs. AUC = 0.817 (p˂0.05)) in the group with a lack or initial signs of liver fibrosis (F0-F2)

    Optimization of Inotropic Support in Victims with Polytrauma and Acute Heart Failure

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    Objective: to evaluate the impact of ultrasound-guided nerve imaging on the efficiency and safety of supraclavicular brachial plexus block. Subjects and methods. Sixty-five patients underwent supraclavicular brachial plexus block. According to the method of nerve identification, all the patients were allocated to one of two groups: 1) Kulenkampff&#8217;s block, by identifying the nerves by a nerve stimulator (n=30); 2) supraclavicular block, by identifying the nerves by ultrasound scanning (n=35). Anesthesia was carried out with a local anesthetic solution containing 20 ml of 2% lidocaine and 10 ml of 0.5% bupivacaine (a total of 30 ml). Results. There is evidence for the high efficiency (97.1%) of ultrasound-guided nerve imaging and its safety (no multiple attempts to verify nerves and complications) as compared to the Kulenkampff supraclavicular block using neurostimulation to identify the plexus (p&lt;0.05). Conclusion. The authors&#8217; modified ultrasound-guided imaging in performing the brachial plexus block helps define nerve localization and observe the placement of a needle against the anatomic structures as it is advanced. Local anesthetic spread observed by ultrasound scanning confirms the precise location of the needle tip. Key words: ultrasound-guided nerve imaging, brachial plexus, efficiency of anesthesia, complication, supra-clavicular approach
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