Origin of the 1 1 5 0 − cm − 1 Raman mode in nanocrystalline diamond

By Andrea C. Ferrari, John Robertson. 2001

1,094 citations recorded by the source corpus.

Subfields: Computational Mechanics, Geophysics, Materials Chemistry

View Paper: https://www.semanticscholar.org/paper/1cdd288e0960a3f9b362c299b2ccd03151b9d8a4

How researchers see this paper

The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.

In Computational Mechanics

1. John Robertson
2. Andrea C. Ferrari
3. Alexander A. Balandin

In Geophysics

1. Andrea C. Ferrari
2. John Robertson
3. Alexander A. Balandin
4. A. Jorio
5. Omid Akhavan
6. C. Charitidis
7. Cinzia Casiraghi
8. S. Rodil

In Materials Chemistry

1. Andrea C. Ferrari
2. Alexander A. Balandin
3. John Robertson
4. F. Rodríguez-Reinoso
5. P. Pendleton
6. K. Kaneko
7. Mark J. Biggs
8. G. Andersson

Citations in the corpus

• Raman spectroscopy of amorphous, nanostructured, diamond–like carbon, and nanodiamond (2004, methodology): “The absolute value of FWHMG decreases with increasing excitation energy and decreases more for more disordered films (Ferrari & Robertson 2001b).”
• Diamond/carbon nanotube composites: Raman, FTIR and XPS spectroscopic studies (2017, background): “Thus, only the spectrum with the 325 nm laser excitation shows the sharp diamond line [37,38].”
• Raman spectroscopy of diamond and doped diamond (2004, background): “Despite very convincing arguments by Ferrari & Robertson (2001), the identification of the peaks at 1460 cm−1 and 1170 cm−1 as due to trans-polyacetylene is still controversial.”
• Thermal properties of graphene and nanostructured carbon materials. (2011, background): “l D~3-5 nm, where thermal transport is controlled by the intrinsic properties of the grain boundaries [49]. The grain boundaries contain sp2-phase as opposed to the sp3-phase carbon inside the grains [54]. Figure 2: Thermal conductivity of disordered and nanostructured carbon materials. (a) K of DLC”
• Raman spectroscopy study of the transformation of the carbonaceous skeleton of a polymer-based nanoporous carbon along the thermal annealing pathway (2015, methodology): “1) at layer edges [42] and, more recently, to zig-zag edges [40,41], although this assignment is questionable given the contrast between the abundance of zig-zag edges in these materials and the relatively low intensity of TPA bands that appear in”