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The absorption, emission, and time decay spectral results evidence the existence of the FRET, the radiative energy transfer (RET), and a synergistic interaction between GQDs and N719 dye.
The decay spectral profiles measured for 4G5/2 → 6H7/2 transition showed single exponential for lower concentration and non-exponential for higher concentration of doped rare earth ion in the as prepared glasses.
Conversion of decay spectral profiles from single to non-exponential have been analyzed using Inokuti Hirayama (I H) model to understand the energy transfer mechanism involved in the decay process.
Sm3+ ions doped Alkaline-Earth Boro Tellurite (AEBT) glasses were prepared by using conventional melt quenching technique and characterized using the spectroscopic techniques such as FT-IR, optical absorption, emission and decay spectral measurements to understand their utility in optoelectronic devices.
The precision of the quantified fat fraction depends on five confounding factors; T1 bias, T2* decay, spectral complexity of fat, noise bias, and eddy currents [ 22].
Otherwise, the application of these ready-available MRI techniques is hindered by the presence of different confounding factors (i.e., T1 relaxation effects, T2* decay, spectral complexity of fat, noise bias, B0 inhomogeneity, and eddy currents), that require proper correction [ 10, 12, 17– 17].
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Using DFA, we have found that Big Dyn induces non-stationary stochastic noise, which has power-law decaying spectral density S f)~1/ f β and asymmetric heavy-tailed single-peak probability density function (all-points histogram) that is indicative of the absence of discreet current levels.
Device measurements included current voltage characteristics, dark current decay, and spectral response.
Once again, we observe that the amplitude fluctuations vary with the observatory magnetic coordinates, viewing a slight decay in spectral exponent fluctuations towards lower latitudes (HER compared with THL).
The obtained decay-associated spectral components show clear differences of the peak energy of 20 to 30 meV between the slowest component (τ1) and the faster two components (τ2, τ3).
To get more quantitative information about lignin homogeneity, the fluorescence decay and the spectral data were evaluated for two different regions of the spectral and FLIM image: one close to an external border (magenta spot) and another in the middle part of the cell wall (blue spot).
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