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The quantization codebook is randomly generated for each quantization process, and we analyze performance averaged over all such choices of random codebooks, in addition to averaging over the fading distribution.
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Given the fast game dynamics, this choice of random directions is probably a consequence of the cognitive limitations in identifying the optimal locations.
This assumption is reasonable by virtue of the approximate rotational symmetry of the eigenvector distribution under our choice of random graph model, which we expect to be close (heuristically) to the eigenvector distribution of the symmetric Gaussian ensemble [19, 20].
This choice of random matrices is motivated by the observation that the distribution of in-degrees and out-degrees in C. elegans is significantly different from Poisson, which is expected for a randomly generated matrix without any correlations (Erdõs-Rényi random graph).
This might be considered remarkable, bearing in mind the high false positive rates of the DL method which have been shown repeatedly with simulations [ 4- 14] and also an empirical study suggesting that results are sensitive to the choice of random effects analysis method [ 26].
Different choices of the random variables T and Y lead to different families of generalized R-distributions.
For this reason, different families of the T-R{generalized lambda} distributions can be derived based on the choices of the random variables T and R. Some general properties of T-R{generalized lambda} families of distributions are studied.
Economic analysis of individual discrete choices makes use of random utility theory [62, 63].
The choice of a random intercept logistic regression model was motivated by both the data structure and the level of measurements of the dependent variable.
In terms of implementation (Kaveh and Bakhshpoori 2013), the generation of numbers with LF consists of two steps: the choice of a random direction and the generation of steps, which obey the chosen Lévy distribution.
As noticed in Bonnefoy-Claudet et al. (2008), A 0HV are larger than A 0HV which is due to the choice of pure random orientation of excitation forces at the surface.
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