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We consider the laser pulse as expressed by Eq. (7), and using Gaussian function for the chirp profile as [32] ω = ω 0 + Δ Exp - ( ξ - ξ 0 ) 2 / σ z 2, in which ω 0 + Δ is frequency at the center of the laser pulse, Δ was called Gaussian chirp parameter and Gaussian chirp width set equal to the spatial duration of the laser pulse (Eq. 7).
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There are frequencies at play and physical energies shifting that do more than merely caramelise your vital organs.
Scores are frequencies at the level of indicators, and not at hospital level, to avoid excluding hospitals with missing values from the analyses.
Thus, the oxidation current is dependent on scan frequency at CFMEs but is frequency independent at CNTYMEs.
Suppression was frequency specific at all ISIs tested (up to 300 ms).
Here, (Gp/ω peak is the maximum Gp/ω value and f0 is the frequency at which this maximum is obtained.
where fmax is the frequency at which the imaginary component of impedance is maximum.
where f n is the frequency at the n-th frequency index.
τ M = 1/2πf max, where f max is the frequency at peak maximum.
The crossover frequency (f co ) is the frequency at which the conductivity independent turns to conductivity dependent.
The signal frequency is at (angular) frequency ω 1, and the pump frequency is ω 3. The amplitudes are arbitrary.
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CEO of Professional Science Editing for Scientists @ prosciediting.com