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A possible consequence of forging in common steels is the apparition of a grain size gradient in the width of the component.
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The spherical scatter width of the components was also taken into account as an optimization parameter.
Thus, de Broglie-Bohm trajectories will partake of the classical motions on the level defined by decoherence (the width of the components).
Width of the components, and the ratio contribution of Gaussian-Lorentzian distribution for certain atoms of the tested samples in the process of spectrum deconvolution were fixed.
To this end, the PL spectrum has been deconvoluted into six Gaussian components in Figure 5a; the centre wavelength, intensities, and half-widths of the component peaks along with their respective uncertainties are given in Table 1.
The depth parameter measurement will be dominated by the shorter correlation time component of the spectra because of the large amplitude and small line width of this component.
For the material with a starting basal texture, heat treatment in the upper α2, (α2+β) or β phase fields does not change the basic character of the texture, although the sharpness and especially the width of the basal component increase to some extent with the increase in the heat treatment temperature.
The width of the narrow component is 1.9 2.7 km and the equivalent depth is about 0.42 km, which corresponds to the normal optical depth of about 0.16 0.25.
The width of the narrow component is 4.1 6.1 km and the equivalent depth is about 2.2 km, which corresponds to a normal optical depth of about 0.3 0.6.
As shown in Fig. 2(a), the width of the dynamic component of the autocorrelation function is assumed to be inversely proportional to velocity.
Similarly, as shown in Fig. 2(b), the width of the dynamic component of the power spectral density (Δf) is assumed to be proportional to velocity.
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