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. 2019 Jun 3;10:2391. doi: 10.1038/s41467-019-10394-8

Table 1.

Different characterization techniques for identifying pure crystalline CNDs

Techniques Crystalline CNDs Amorphous CNDs Crystalline quasi CNDs Aggregated fluorophores
HR-TEM

a. Size 2–5 nm,

b. Lattice fringes

c. Interlayer spacing of 0.34 nm for 002 plane

d. Interlayer spacing of 0.21 nm for 001 plane

a. Size 2–5 nm,

b. No lattice fringes

c. No interlayer spacing

a. Size 2–5 nm,

b. Lattice fringes

c. Interlayer spacing of 0.34 nm for 002 plane

d. Interlayer spacing of 0.21 nm for 001 plane

Almost similar to CNDs. A little variation may be observed based on the fluorophore structure
XRD Sharp peak at ~24˚ for 002 plane Broad peaks as compared to CND/Quasi CND Sharp peak at ~24˚ for 002 plane Sharp peak at ~24˚ for 002 plane
AFM The height profile will confirm the size of 2–5 nm, topology and number of graphene layers in CNDs The height profile will confirm the size of 2–5 nm and topology The height profile will confirm the size of 3–5 nm, topology and number of graphene layers in CNDs The height profile will confirm the size of 2–5 nm and topology
Raman Spectroscopy

a. Sharp G band at ~1580 cm−1,

b. 2D band at ~2680 cm−1

c. less intense D band ~1360 cm−1 due to edge defect by surface functional groups

Predominant broad D bands or high D/G ratio Same as CNDs as it contains the same crystalline core Almost similar to CNDs. A little variation may be observed based on the fluorophore structure
TGA No mass loss and mostly stable up to 800 °C No mass loss and mostly stable up to 800 °C Due to less thermal stability of molecular fluorophore extensive mass loss within 300 °C Due to less thermal stability of molecular fluorophore extensive mass loss within 300 °C
Confocal Raman PL Due to high thermal stability of carbon core no change in PL intensity at lower temperature ~300 °C Due to high thermal stability of carbon core no change in PL intensity at lower temperature ~300 °C Due to less thermal stability of molecular fluorophore huge reduction in PL intensity within 300 °C Due to less thermal stability of molecular fluorophore complete reduction in PL intensity within 300 °C