Here we review the aspects of the SLSTR instrument design specifically targeted at biomass burning events, including operation of the SWIR channels at night and the inclusion of low-gain middle infrared and thermal IR channels that will minimise saturation over even high intensity fires.
Biophysical characteristics of the species vary based on peat depth, soil saturation, and fire history.
In the model used here, a stimulus will drive equation (1) into saturation of firing rates quickly.
The nonlinear function Θ x), typically a sigmoid of hyperbolic-tangent type, limits the growth of its argument to an asymptotic value which accounts for the saturation of firing rates in real neurons.
The traces are shown until the firing reached saturation.
Moreover, if, as suggested in the subsection "PVs and SOMs differentially suppress putative excitatory neuron responses to standard and deviant tones", SOM neurons are firing at saturation to deviant tones, the authors should have the data to show this.
Because those fluctuations are not sufficiently strong to evoke large variations of the firing rate, the saturation due to the nonlinear function Θ can be ignored in the study of spontaneous activity.
A similar protocol was used by Schreiber et al. [116] to measure PS II photoinhibition caused by the toxic effects of diuron, suggesting that since quantum yields are calculated from the ratio of fluorescent values before (Ft) and after (Fm') firing a constant saturation pulse, results are independent of signal amplitudes.
For large values, typically too much activity was propagated, making it more difficult to distinguish the responses of the output neurons to each stimulus as the firing rates approached saturation point.
Core/shell ferrite nanoparticles show lower magnetization saturation than the uncoated ferrite nanoparticles fired at the same temperature, while the switching field increases for the coated ferrite nanoparticles.
