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33 eV) from a Nd:YVO4 laser for 180 min. The irradiation power level in a focal spot of 1 μm in diameter on the sample was kept at ~20 mW. 5×10−4 Pa, respectively. 2. Change in D band by heating Figure 7 shows D and G bands in the Raman spectrum for a pristine CoMoCAT SWCNT sample. The corresponding radial breathing modes (RBMs) are also shown in the inset in the figure. The spectral peaks are fitted with Lorentzian lines. 8 nm, which cor‐ responds to typical mean diameter of CoMoCAT ones [27].

Journal of Materials Chemistry. 2002;12:2762-8. [19] Karanikas S, Louis AA. Dynamic Colloidal Stabilization by Nanoparticle Halos. Physical Review Letters. 2004;93:248303. [20] Vaisman L, Wagner HD, Marom G. The role of surfactants in dispersion of carbon nanotubes. Advances in Colloid and Interface Science. 2006;128–130:37-46. [21] Hilding J, Grulke EA, George Zhang Z, Lockwood F. Dispersion of Carbon Nano‐ tubes in Liquids. Journal of Dispersion Science and Technology. 2003;24:1-41. [22] Keblinski P, Eastman JA, Cahill DG.

Numerical Heat Transfer, Part A: Applications. 2007;52:1043-58. 5772/51965 [90] Behzadmehr A, Saffar-Avval M, Galanis N. Prediction of turbulent forced convection of a nanofluid in a tube with uniform heat flux using a two phase approach. Interna‐ tional Journal of Heat and Fluid Flow. 2007;28:211-9. [91] Mohammed HA, Bhaskaran G, Shuaib NH, Abu-Mulaweh HI. Influence of nano‐ fluids on parallel flow square microchannel heat exchanger performance. Interna‐ tional Communications in Heat and Mass Transfer.

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