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The difference in the latency of activation (defined as the time of the peak of the PSTH, compare also Sakata and Harris 2009) between the input layers and the output layers in our network is with around 2 3 ms below the experimentally observed latencies (5 10 ms according to Schroeder et al. (1998); Sakata and Harris (2009)).
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As in synapse formation experiments, 6, 8, 15 our model did not produce synapses below this critical value of BCR/Ag affinity, thereby matching the experimentally observed affinity range of synapse formation.
To match this output to the experimentally observed fluorescence data, we performed the fitting procedure as described below in the section titled "Fitting procedure for fluorescence".
Vertical arrows indicate the experimentally observed transitions.
The theoretical and the experimentally observed signals have been compared.
The experimentally observed relaxation strength in a time of approximately 3 h at 50 K below Tg is of the order of 40 60%.
The calculations compare favorably with the experimentally observed identity probabilities.
The models have been compared with the experimentally observed accelerations later in the paper.
Figure 9a c depict the experimentally observed load-displacement response curves of the presented test specimens.
The results from the thermal model were validated from the experimentally observed data.
The obtained computational results provide a possible explanation for the experimentally observed high diastereoselectivity.
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Justyna Jupowicz-Kozak
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