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The data shows the photodetachment induced depletion as a function of probing the ion packet at different distances from the mirror towards the ion source (negative delays).
The values were obtained at positive and negative delays, and statistically significant covariance function values were averaged for delays of 0 and +/− 1 2, 3 4, 5 6, 7 8, and 9 10 ms (Fig. 7, top, shows an example of this procedure).
Finally, in cells from superficial layers, positive and negative delays were nearly equally frequent, and the spread of delays was high.
A delay of 1 s increases LTP, whereas delays of 0 or 200 ms fail to elicit LTP, and negative delays induce LTD.
Population analysis of activity onset estimated with both methods revealed that neurons recorded in deep layers were leading, as indicated by high occurrence of negative delays in these cells as compared with superficial layer neurons (Fig. 6 a, d ).
Similar(55)
The positive and negative values indicate positive and negative delay times from each origin time, respectively.
By contrast, a negative delay denotes that the beginning of the estimative phase is earlier than it really is.
The degrees differ depending on the computation algorithms; in particular, BFMF had opposite tendencies to ARG and BFMP toward over- and underestimation for positive and negative delay times.
The delay times are presented with a step of 3 min, excluding events with zero and negative delay time, the latter events being united in one group irrespective of the actual negative value of ΔT.
Our data reveal that the strong negative delay effect can be explained in large part by narrow bracketing and the increased perceived complexity of the environment, rather than by time discounting per-se.
The average delay time of all the events was -29 s (the median is -35 s), with 87% of events showing negative delay times that indicate that the Pi 2 pulsations at ETS-VIII occurred before the Pi 2 at KUJ. Figure3c shows the local time dependence of the delay times between ETS-VIII and KUJ.
Related(20)
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