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. 2017 Mar 7;8(5):3538–3546. doi: 10.1039/c6sc04903f

Fig. 3. (a) Wide-angle PXRD patterns, (b) Raman spectra, and (c) N2 adsorption–desorption isotherms of the non-hollow carbon nanoparticles and hollow carbon nanobubbles. The pore size distribution of the hollow carbon nanobubbles is calculated by the non-local density functional theory (NLDFT) method, as shown in the inset of (c).

Fig. 3