18,239 research outputs found

    Blood oxygen saturation determined by transmission spectrophotometry of hemolyzed blood samples

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    Use of the Lambert-Beer Transmission Law determines blood oxygen saturation of hemolyzed blood samples. This simplified method is based on the difference in optical absorption properties of hemoglobin and oxyhemoglobin

    Improved sample capsule for determination of oxygen in hemolyzed blood

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    Sample capsule for determination of oxygen in hemolyzed blood consists of a measured section of polytetrafluoroethylene tubing equipped at each end with a connector and a stopcock valve. This method eliminates errors from air entrainment or from the use of mercury or syringe lubricant

    The Geography of Output Volatility

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    This paper examines the structural determinants of output volatility in developing countries, and especially the roles of geography and institutions. We investigate the volatility effects of market access, climate variability, the geographic predisposition to trade, and various measures of institutional quality. We find an especially important role for market access: remote countries are more likely to have undiversified exports and to experience greater volatility in output growth. Our results are based on Bayesian methods that allow us to address formally the problem of model uncertainty and to examine robustness across a wide range of specifications.Volatility, Geography, Institutions, Bayesian Model Averaging

    Efficient separation of the orbital angular momentum eigenstates of light

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    Orbital angular momentum (OAM) of light is an attractive degree of freedom for funda- mentals studies in quantum mechanics. In addition, the discrete unbounded state-space of OAM has been used to enhance classical and quantum communications. Unambiguous mea- surement of OAM is a key part of all such experiments. However, state-of-the-art methods for separating single photons carrying a large number of different OAM values are limited to a theoretical separation efficiency of about 77 percent. Here we demonstrate a method which uses a series of unitary optical transformations to enable the measurement of lights OAM with an experimental separation efficiency of more than 92 percent. Further, we demonstrate the separation of modes in the angular position basis, which is mutually unbiased with respect to the OAM basis. The high degree of certainty achieved by our method makes it particu- larly attractive for enhancing the information capacity of multi-level quantum cryptography systems

    Geometrical Aspects Of BRST Cohomology In Augmented Superfield Formalism

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    In the framework of augmented superfield approach, we provide the geometrical origin and interpretation for the nilpotent (anti-)BRST charges, (anti-)co-BRST charges and a non-nilpotent bosonic charge. Together, these local and conserved charges turn out to be responsible for a clear and cogent definition of the Hodge decomposition theorem in the quantum Hilbert space of states. The above charges owe their origin to the de Rham cohomological operators of differential geometry which are found to be at the heart of some of the key concepts associated with the interacting gauge theories. For our present review, we choose the two (1+1)(1 + 1)-dimensional (2D) quantum electrodynamics (QED) as a prototype field theoretical model to derive all the nilpotent symmetries for all the fields present in this interacting gauge theory in the framework of augmented superfield formulation and show that this theory is a {\it unique} example of an interacting gauge theory which provides a tractable field theoretical model for the Hodge theory.Comment: LaTeX file, 25 pages, Ref. [49] updated, correct page numbers of the Journal are give

    Production of (τ+τ)b(\tau^+\tau^-)_b in electron positron collisions

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    (τ+τ)b(\tau^+\tau^-)_b is an atom of simple hydrogenlike structure similar to positronium (e+e)b(e^+e^-)_b and (μ+μ)b(\mu^+\mu^-)_b. In this paper energy levels and decay widths of different decay channels of (τ+τ)b(\tau^+\tau^-)_b are given. Cross section of production of this atomic system in e+ee^+e^- annihilation taking into account radiative corrections is calculated. According to our estimates 886 (τ+τ)b(\tau^+\tau^-)_b atoms may be produced at BEPCII and 29 (τ+τ)b(\tau^+\tau^-)_b atoms are produced at VEPP-4M under the present experimental conditions.Comment: 5 pages, submitted to Int. Jour. Mod. Phys.

    Nonmodal energy growth and optimal perturbations in compressible plane Couette flow

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    Nonmodal transient growth studies and estimation of optimal perturbations have been made for the compressible plane Couette flow with three-dimensional disturbances. The maximum amplification of perturbation energy over time, GmaxG_{\max}, is found to increase with increasing Reynolds number Re{\it Re}, but decreases with increasing Mach number MM. More specifically, the optimal energy amplification GoptG_{\rm opt} (the supremum of GmaxG_{\max} over both the streamwise and spanwise wavenumbers) is maximum in the incompressible limit and decreases monotonically as MM increases. The corresponding optimal streamwise wavenumber, αopt\alpha_{\rm opt}, is non-zero at M=0, increases with increasing MM, reaching a maximum for some value of MM and then decreases, eventually becoming zero at high Mach numbers. While the pure streamwise vortices are the optimal patterns at high Mach numbers, the modulated streamwise vortices are the optimal patterns for low-to-moderate values of the Mach number. Unlike in incompressible shear flows, the streamwise-independent modes in the present flow do not follow the scaling law G(t/Re)Re2G(t/{\it Re}) \sim {\it Re}^2, the reasons for which are shown to be tied to the dominance of some terms in the linear stability operator. Based on a detailed nonmodal energy analysis, we show that the transient energy growth occurs due to the transfer of energy from the mean flow to perturbations via an inviscid {\it algebraic} instability. The decrease of transient growth with increasing Mach number is also shown to be tied to the decrease in the energy transferred from the mean flow (E˙1\dot{\mathcal E}_1) in the same limit
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