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mean probe delay.
In [19], mean probe delay (MPD) was proposed and used as an indicator of an AP's load.
While still leading to errors up to 10% at worst, the empirically determined Raman linewidth factors eliminated any systematic error in the O2/N2 measurements with probe delay.
Using the transient absorption signal at a specific probe delay as feedback, the triplet signal could be optimized over the singlet contribution.
Robustness against linear and nonlinear absorption artifacts is achieved by detecting the spectral shifting with a balanced photodiode and linear projection of acquired data onto a reference XPMSS probe delay scan.
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At a mean chamber pressure of 1.39 MPa evaluated mean particle diameters increased by a factor of two for probe delays between 5 and 16 ms after start of injection irrespective of the choices of first-guess fitting variables, indicating a certain robustness of data analysis procedure.
Longer probe delays, required for improved dynamic range in regions of high temperature fluctuations, proved difficult to model as a result of a nontrivial decay in the O2 Raman coherence arising from complexities associated with the triplet ground electronic state of the O2 molecule.
Figure 2 Pump-probe delay dependence of the PSSHG for a typical sample.
Figure 2 shows the pump-probe delay dependence of the PSSHG signal for a typical sample (1.2 nm; 0.8% Cu).
The transient reflectivity change ΔR/R of the probe beam was measured as a function of the pump-probe delay time.
More importantly, we also found patterns of proactive control activity (i.e., changes in activation during the pre-probe delay period resulting from interference expectancy) in several regions previously implicated in WM.
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