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Fourier spectrum of uniform sampling.
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To further discuss the extinction spectra results, we used the FDTD method to calculate the extinction spectra of uniform and nonuniform nanoarrays (Figure 2c).
Two set of peaks were observed in 1H 15N HSQC spectrum of purified, uniform 15N-labeled reduced sample, such as the side chain peak of W82 (Fig. 2A).
An analytical procedure to investigate the response spectrum of a uniform Bernoulli-Euler beam with axial compressive load subjected to random support excitations is implemented based on the Mindlin-Goodman method and the mode superposition method in the frequency domain.
In solving direct problems, it is shown that the spectrum of non-uniform composite beams can be obtained with fair accuracy.
First, we determine completely the spectrum for uniform K1(3 -GDDs of type gu.
We prove that instability of pure point spectrum implies absence of uniform localization.
We then use it to obtain a lower bound on the spectrum in terms of uniform or Lp bounds on the curvature and current of the connection.
The PL spectra of the uniform InAs QDs revealed a narrow linewidth of less than 26 meV.
(c) Simulation extinction spectra of the uniform and nonuniform Au nanoarrays with period a = 110 nm and diameter d = 34 nm.
The cross-peaks in the HSQC spectrum for IκBα 67−206) were generally of uniform intensity, indicative of a well-structured protein unlike the that seen for IκBα 67−287) (40).
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