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If this is the case, it will inherit the final peak label from this key peak.
The binding energies of the Fe 2p3/2 peak (label A) and Fe 2p1/2 peak (label B) for the c (4 × 8) phase are 706.8 and 719.7 eV, respectively.
Now we propagate the final peak label through the key saddles in a level-by-level fashion.
Every peak is assigned a 'final peak' label which is initialized to the peaks own peak ID and updated whenever a peak is merged to another one.
On each level, we iterate until no final peak label is moved, while the virtual boundaries are updated after every iteration.
We have simply replaced cells by peaks, densest neighbour cells with key neighbours and the peak patch label by the final peak label.
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In particular, the peak labeled C in this report decreases in intensity with graphitization and the peak position steadily moves to the negative direction in the potential range of 0.16 to 0.25 V (versus Li/Li+).
The peak labels correspond to the labels in Figs 5 and 6. Figure 5: The products obtained from the linear structures with symbolic numbers corresponding to the GC/MS spectrograms in Fig. 4. Figure 6: The products obtained from the ring structures with symbolic numbers corresponding to the GC/MS spectrograms in Fig. 4.
The peak labeled with asterisk is CuK peak originating from the TEM grid.
The peak labeled with asterisk is ascribed to the Al2O3 (1120) diffraction plane (JCPDS Cards no.: 43 1484).
When R is equal to 1, the shorter wavelength peak, labeled as peak 1, is strong and shows a blueshift effect.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com