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While similar acoustic performances are observed over most part of the spectrum, noticeable improvements can be found in the low frequency regime, i.e. below 500 Hz.
We start our analysis with the most noticeable feature noticed in the spectra.
Grain boundary contribution to total electrical conductivity was not noticeable in impedance spectra of low temperature phase, while it shows up at high temperature phase.
This was particularly noticeable in the spectra of histones H4 and H2B.
Fig. 4 EPR spectra of Mn-doped ZnSxSe1−x NCs with short (15 min) and long (60 min) growth times before (the dashed lines indicate peak-to-peak position of the broad isotropic resonance) and after surface exchange/passivation. Inset magnifies the maximum intensity region for the short and long growth times with the short growth time spectrum showing noticeable hyperfine splitting.
The modes are densely spaced in frequency, but for both materials there is a noticeable "gap" in the spectrum between the 9th and 10th modes as indicated by the red arrows in Fig. 1 (the higher red arrow links the positions of the highest-frequency Raman-active modes).
In addition, a weak feature at 316 cm–1 in this region is noticeable in the simulated spectrum but is absent in the experimental NRVS data.
General similarities of the spectra are noticeable, although subtle variations of relative peak heights are also present, which indicates that some infrared (IR) absorbers are not parallel.
The PL spectra indicate noticeable decrease of the integrated intensity for both types of irradiated PTDs with the increase of electron beam doses.
Fluorescent NPs possessed many advantages, including photo-stability, wide absorption and narrow emission spectra, more noticeable size-dependent Stokes shifts, robust stability against photo-bleaching and chemical degradation, higher fluorescent quantum yield, high sensitivity, and large molar extinction coefficients [16 18].
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CEO of Professional Science Editing for Scientists @ prosciediting.com