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For two peaks, (107) and (01.11), the intensity is too low to be resolved.
It can be seen from Figure 5a that the RWT can detect the LFM signal for two peaks around the chirp rate.
We first define a positive metric for two peaks p n and q m : d n, m = p n − q m, (3).
In order to investigate the origin of first and second peaks, we have investigated the dependences of the intensities for two peaks of SAQDs on the excitation power of laser.
For T NOE =2,the correct assignment was not established for two peaks (a swap of assignment possibilities: residue 207↔208) without being detected.
We also noted that the number of SVs decreased rapidly with increasing size, except for two peaks corresponding to short and long interspersed nuclear elements (SINEs and LINEs) around 200 bp and 2000 bp, respectively.
Similar(54)
From the obtained dependencies, the real part of the cubic NLO susceptibility was calculated for two peak laser intensity ranges: (i) 25 50 MW/cm2 and (ii) 190 240 MW/cm2.
Obviously, under the same conditions, the red shifts for three peaks were different.
In order to detect rectangles, they search through Hough domain for four peaks which satisfy certain geometric conditions, such that they represent two perpendicular pairs of parallel intersecting lines.
This concept is illustrated for three peaks of EIN HSQC in Figure S1.
Shown in Figure 4a are the intensities for three peaks as a function of exit gate opening time.
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