Using a threshold value of 10U/ml,the sensitivity of NMP22 was 87. 5% with the specificity of 71. 9%, the positive predictive value of 75. 5% and the negative predictive value of 85. 2%.
We show that the structure of a block outside the critical hyperplanes of category O over a symmetrizable Kac-Moody algebra depends only on the corresponding integral Weyl group and its action on the parameters of the Verma modules.
We also prove the uniqueness of Verma embeddings outside the critical hyperplanes.
Using the matrix approach we prove that the sequence of sampling functions is always complete in the cases of critical sampling and oversampling.
An important example is the Moser-Trudinger inequality where limiting Sobolev behavior for critical exponents provides significant understanding of geometric analysis for conformal deformation on a Riemannian manifold [5, 6].
On Generating Tight Gabor Frames at Critical Density
We show that the structure of a block outside the critical hyperplanes of category O over a symmetrizable Kac-Moody algebra depends only on the corresponding integral Weyl group and its action on the parameters of the Verma modules.
We also prove the uniqueness of Verma embeddings outside the critical hyperplanes.
When β is less than some critical value the boundary periodic solution (xs(t), 0, zs(t)) is locally stable, and when β is larger than the critical value there are periodic oscillations in substrate, prey and predator.
The critical micelle concentration (cmc) and surface tension of the novel zwitterionic Gemini surfactant in aqueous solution at 15°C are 7.2×10-5 mol/L and 34.5 mN/m, respectively.
Then, from the curves, the critical micelle concentration (CMC) and the thermodynamic standard formation functions (ΔH?m, ΔG?m and ΔS?m) were obtained through thermodynamic theories.
Using the matrix approach we prove that the sequence of sampling functions is always complete in the cases of critical sampling and oversampling.
At last, we discuss the series expressions of these functions and give a Box-counting dimension estimation of "critical" fractal interpolation functions by using our smoothness results.
there exists a C∞ rank-1 map f: I2→R1 such that f(A) has nonempty interior for some subset A ?I2 of critical points with finite Hausdorff dimension.
The modeling of defect outlines that exhibit a great variety of defect shapes is usually modeled as a circle, which causes the errors of critical area estimation.
The dependences of critical current density Jc on the interlayer coupling strength and magnetic field in Bi2212 crystals were obtained by measuring the magnetic loop of the crystals with different interlayer coupling strengths.
The MCA algorithm consists of an iterative alternating projection and thresholding scheme, using a successively decreasing threshold towards zero with each iteration.
The system is subject to failure and it fails once the total cumulative damage level first exceeds a fixed threshold.
The Merris' conjectures for threshold graphs and d-regular graphs are proved.
For two important special cases of mass action incidence and standard incidence, global stability of the endemic equilibrium is proved provided the threshold is larger than unity.
The relationship between the order of approximation by neural network based on scattered threshold value nodes and the neurons involved in a single hidden layer is investigated.
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