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They detected lines in emission spectra that corresponded to highly polarized light and that split into multiple peaks when magnetic fields were applied.
Fig. 7 Periodic function g with multiple peaks when there is an asymmetry in the common extrinsic noise source to the excitatory and inhibitory populations.
In the case of stochastic E-I limit cycle oscillators, we were unable to find a parameter regime where g develops multiple peaks when the common extrinsic noise source is the same for both excitatory and inhibitory populations, that is, χ E = χ I = 1 / 2 in equations (14) and (17).
However generally, ITS is highly variable, with indels and paralogues which caused multiple peaks when directly sequenced (unpublished results).
Having done this, we integrated data from multiple peaks (when present) to generate a gene-level metric of ChIP signal in each individual.
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However, multiple peaks can occur when there is an asymmetry between the excitatory and inhibitory stochastic drives, as illustrated in Figure 7.
One possible explanation is that multiple peaks are formed when the source of the gamma-ray burst undergoes precession.
The latter measure is more robust than time to epidemic peak, when multiple peaks are observed.
Interesting findings include the appearance of internal resonance peaks when multiple beam modes are considered.
When multiple peaks are close together, interference between adjacent columns can create amplitude or phase images that appear to break the radial symmetry.
Gravity or center frequency is more appropriate when multiple peaks are detected in the alpha range (Klimesch, 1999).
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