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Adaptive thresholds

Figure A3.12.8. Possible absorption spectrum for a molecule which dissociates via isolated compound-state resonances. Eq is the unimolecular threshold. (Adapted from [4].)... Figure A3.12.8. Possible absorption spectrum for a molecule which dissociates via isolated compound-state resonances. Eq is the unimolecular threshold. (Adapted from [4].)...
Fig. 3.1. Recapitulation of the inner nodes for radial Coulomb wavefunctions also shown are the near-threshold continuum function with delta function normalisation (dotted curve) and two continnum functions above the threshold (adapted from H. Friedrich [112]). Fig. 3.1. Recapitulation of the inner nodes for radial Coulomb wavefunctions also shown are the near-threshold continuum function with delta function normalisation (dotted curve) and two continnum functions above the threshold (adapted from H. Friedrich [112]).
Figure 22.12 Top poLenLialenergyatthecriLicalconfig-uration as a function of orienLation angle 7c. Bottom reactive spot fortwo reactive siLuaLions (a) at collision energy near threshold and (b) well above threshold. Adapted from Loesch, in Ldseresy Reacciones Qui micas (1989)... Figure 22.12 Top poLenLialenergyatthecriLicalconfig-uration as a function of orienLation angle 7c. Bottom reactive spot fortwo reactive siLuaLions (a) at collision energy near threshold and (b) well above threshold. Adapted from Loesch, in Ldseresy Reacciones Qui micas (1989)...
Fig. 7 Scaled characteristic diffusion time of fluorescent TAMRA molecules in PVA solutions and gels at several crosslink densities as a function of polymer concentration with linear fits. The times are scaled by the diffusion time of the probe in water. The vertical dashed line indicates the approximate gelation threshold (adapted from Michehnan-Ribeiro et al. [127])... Fig. 7 Scaled characteristic diffusion time of fluorescent TAMRA molecules in PVA solutions and gels at several crosslink densities as a function of polymer concentration with linear fits. The times are scaled by the diffusion time of the probe in water. The vertical dashed line indicates the approximate gelation threshold (adapted from Michehnan-Ribeiro et al. [127])...
At first, it is statistical standard of the undefective section. Such standard is created, introducing certain lower threshold and using measured data. Under the classical variant of the shadow USD method it is measured fluctuations of accepted signal on the undefective product and installed in each of 512 direction its threshold in proportion to corresponding dispersions of US signal in all 128 sections. After introducting of threshold signal is transformed in the binary form. Thereby, adaptive threshold is one of the particularities of the offered USCT IT. [Pg.249]

Threshold, Saturation, and Adaptation. Several aspects of flavor perception are not accounted for in the Weber-Stevens laws, eg. [Pg.2]

The odor detection-threshold values of organic compounds, water, and mineral oil have been determined by different investigators (Table 2 and 3) and may vary by as much as 1000, depending on the test methods, because human senses are not invariable in their sensitivity. Human senses are subject to adaption, ie, reduced sensitivity after prolonged response to a stimulus, and habituation, ie, reduced attention to monotonous stimulation. The values give approximate magnitudes and are significant when the same techiriques for evaluation are used. Since 1952, the chemistry of odorous materials has been the subject of intense research (43). Many new compounds have been identified in natural products (37—40,42,44—50) and find use in flavors. [Pg.11]

Data that is not evenly distributed is better represented by a skewed distribution such as the Lognormal or Weibull distribution. The empirically based Weibull distribution is frequently used to model engineering distributions because it is flexible (Rice, 1997). For example, the Weibull distribution can be used to replace the Normal distribution. Like the Lognormal, the 2-parameter Weibull distribution also has a zero threshold. But with increasing numbers of parameters, statistical models are more flexible as to the distributions that they may represent, and so the 3-parameter Weibull, which includes a minimum expected value, is very adaptable in modelling many types of data. A 3-parameter Lognormal is also available as discussed in Bury (1999). [Pg.139]

Algorithm 1 requires the a priori selection of a threshold, s, on the empirical risk, /en,p( X which will indicate whether the model needs adaptation to retain its accuracy, with respect to the data, at a minimum acceptable level. At the same time, this threshold will serve as a termination criterion for the adaptation of the approximating function. When (and if) a model is reached so that the generalization error is smaller than e, learning will have concluded. For that reason, and since, as shown earlier, some error is unavoidable, the selection of the threshold should reflect our preference on how close and in what sense we would like the model to be with respect to the real function. [Pg.178]

The multiscale basis functions capture the fast changes in coefficients corresponding to the fine-scale basis functions, while the slower changes are captured by the coarse-scale basis functions. Thus, the wavelet thresholding method adapts its resolution to the nature of the signal features and reduces the contribution of errors with minimum distortion of the features retained in the rectified signal. [Pg.22]

Fig. 16. Phototropic threshold of wild type and hypothetical photoreceptor mutants. Solid line = wild type large dashes = mutant with reduced number of photoreceptor dotted line = mutant with reduced absorption cross-section small dashes = mutant with slow regeneration. The changes of threshold of the hypothetical mutants were chosen arbitrarily. The figure was adapted to Fig. 6 and the solid line of the wild type represent data of Foster and Lipson (1973)... Fig. 16. Phototropic threshold of wild type and hypothetical photoreceptor mutants. Solid line = wild type large dashes = mutant with reduced number of photoreceptor dotted line = mutant with reduced absorption cross-section small dashes = mutant with slow regeneration. The changes of threshold of the hypothetical mutants were chosen arbitrarily. The figure was adapted to Fig. 6 and the solid line of the wild type represent data of Foster and Lipson (1973)...
Figure 11. C2H4 ion yield as a function of time in femtoseconds for a pump-photoionization probe experiment. Heavy line Predicted ion yield using the AIMS data and assuming an ionization threshold of 3.5eV. Dashed line Exponential fit to the AIMS ion yield predicting an excited state lifetime of 35 fs. Gray shaded area Reported ion yield [152] obtained using an exponential fit to the experimental data predicting an excited state lifetime of 30 15 fs. (Figure adapted from Ref. 214.)... Figure 11. C2H4 ion yield as a function of time in femtoseconds for a pump-photoionization probe experiment. Heavy line Predicted ion yield using the AIMS data and assuming an ionization threshold of 3.5eV. Dashed line Exponential fit to the AIMS ion yield predicting an excited state lifetime of 35 fs. Gray shaded area Reported ion yield [152] obtained using an exponential fit to the experimental data predicting an excited state lifetime of 30 15 fs. (Figure adapted from Ref. 214.)...

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Threshold adaptive system mode dependent

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