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We find: (i) some common solutes in commercial Al alloys (e.g., Cu and Mg) possess either very weak (Cu), or even repulsive (Mg), binding energies.
This indicates that some weak Cu filaments are broken during read pulse endurance at a high value of negative voltage.
These large crystallites are sufficient to provide a good coloration to the paint, but have been found [38], to contribute to low intensity emissions, when probed by LIBS, and this may explain weak Cu emission lines observed in the dark green paint area of AI244.
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The weak interactions between Cu and graphene, along with the low solubility of carbon in Cu, make Cu particles ideal for tracking their etching paths on graphene.
The three specimens inoculated with bacteria showed weak shoulder of Cu-carboxylate complexes at 1585 cm−1.
Cu interlayer facilitated the graphitic rearrangement in bilayer films due to weak Cu/C bonds and Cu surface layer could be more effective against graphitization.
In addition, on the basis of the Raman spectrum in Figure 1 c, RBMs were detected in the rebar graphene sheets; the intensity ratio of the D to G bands dropped to <0.1, demonstrating the weak etching effects of Cu on SWCNTs because of the low solubility of carbon in Cu (<0.001 atom % at 1000 °C).
Research has shown that heat flow in Cu-CNTs is limited by the weak bonds across the Cu-CNT interfaces and that its thermal conductivity is significantly lower than the estimated value for the intrinsic thermal conductivity of the CNTs.
Significant intensity modulation in the resonant XES spectral shape upon different excitation energies near the C K-edge indicates that graphene layer preserves an intrinsic momentum as that of HOPG and the interaction between graphene and Cu shows weak influence on the valence band structure of graphene.
This combination can be attributed to the specific behavior of AC with high surface area and weak interaction between metallic Cu active sites and AC [107, 108].
Although the main five diffraction peaks were indexed to Cu2O (JCPDS: 05 0667), weak diffraction peaks of Cu for [111] and [211] crystal surfaces (JCPDS: 04 0836) appeared from the solid octahedral sample (Figure3a) and hollow octahedral sample (Figure3b).
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