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The conversion function is interpreted as the expectation value of the target spectral envelope.
In this approach, the conversion function is interpreted as the expectation value of the target spectral envelope.
If the function is interpreted as part of a physical model then we are likely to call the device a simulator.
While in the minimal and the non-minimal Bohm theories, the wave function is interpreted as a field, Dürr, Goldstein and Zanghì (1997, section 12) propose that the wave function should be interpreted as a parameter of a physical law.
In this approach, the conversion function is interpreted as the expectation value of the target spectral envelope, and the conversion parameters are evaluated using minimum mean-square error (MMSE) on a parallel training set.
The slope of the search function is interpreted as indicator for the search efficiency for particular target-distractor pairings.
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The structure matrix (specifically, the correlations between each variable and the first discriminant function) was interpreted.
The negative regions of the Wigner function are interpreted as comprised by negative particles, and the particle sign is taken into account when obtaining the physical averages.
Insulin resistance and Beta cell function were interpreted using the homeostasis model analysis (HOMA), as described by [ 29]: (1) HOMA-IR = [ Fasting Insulin (mU / L ) × Fasting Glucose (mmol / L ) ] 22.5 HOMA- β = [ 20 × Fasting Insulin (mU / L ) Fasting glucose (mmol / L ) − 3.5 ].
Boolean functions are interpreted as classification tasks.
The correlation functions were interpreted in terms of a two-phase model to obtain average lamellar and amorphous, layer thicknesses.
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