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Since, both the samples are P53-knockout MEFs, with one of them carrying over expression of Mta1; the differentially expressed genes were regulated by Mta1 independent of P53.
The latter also indicates that both the samples are mesostructured materials.
Regarding the clustering coefficient, we observed that the average values for both the samples are very high, similarly as reported by other recent studies on OSNs [3, 44].
The obtained values of saturation magnetization (M s), remnant magnetization (M r) and coercivity (H c) are given in Table 2 and the M H loops of both the samples are given in Fig. 6.
Comparing PL spectra of samples with InAs coverage of 1.80 MLs and 1.85 MLs, we find the peak positions in PL spectra of both the samples are almost same.
Moreover, the broad bands at 1574 cm-1 for both the samples are assigned to the C = C skeletal vibration of graphene sheets [45], which confirms the successful reduction of GO sheets.
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The TEM imaging of the both the samples was done using Philips TEM model CM200.
Both the samples were observed to be extremely hard (458 471 HV1).
Both the samples were prepared for the same CIGS deposition duration.
The size of both the samples is in the magnitude of few millions of nodes and edges.
This could be attributed to the quality of substrates where both the samples were of a fibrous nature.
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