Optical properties of amorphous carbon thin films prepared by plasma deposition in a graphite hollow cathode

1992 ◽  
Vol 220 (1-2) ◽  
pp. 125-131 ◽  
Author(s):  
Juan Manuel Mendez ◽  
Stephen Muhl ◽  
G. Contreras-Puente ◽  
J. Aguilar-Hernandez
Keyword(s):  
Thin Films ◽  
Optical Properties ◽  
Amorphous Carbon ◽  
Hollow Cathode ◽  
Plasma Deposition ◽  
Carbon Thin Films

Understanding terahertz optical properties of amorphous carbon thin films

Carbon ◽  
2013 ◽  
Vol 64 ◽  
pp. 67-71 ◽  
Author(s):  
H. Wang ◽  
J.Q. Guo ◽  
Y.S. Zhou
Keyword(s):  
Thin Films ◽  
Optical Properties ◽  
Amorphous Carbon ◽  
Carbon Thin Films

Some optical properties of amorphous hydrogenated carbon thin films prepared by rf plasma deposition using methane

2001 ◽  
Vol 32 (9) ◽  
pp. 783-786 ◽  
Author(s):  
Marco A.R. Alves ◽  
Jônatas F. Rossetto ◽  
Olga Balachova ◽  
Edmundo da Silva Braga ◽  
Lucila Cescato
Keyword(s):  
Thin Films ◽  
Optical Properties ◽  
Plasma Deposition ◽  
Rf Plasma ◽  
Carbon Thin Films ◽  
Amorphous Hydrogenated Carbon

Correlation of structural and optical properties of PVD grown amorphous carbon thin films

2017 ◽  
Vol 75 ◽  
pp. 69-77 ◽  
Author(s):  
Infant Solomon ◽  
Mukul Bhatnagar ◽  
Krishnanand Shukla ◽  
Bornali Sarma ◽  
Mukesh Ranjan ◽  
...  
Keyword(s):  
Thin Films ◽  
Optical Properties ◽  
Amorphous Carbon ◽  
Structural And Optical Properties ◽  
Carbon Thin Films

Electron-diffraction studies of amorphous carbon thin films

1993 ◽  
Vol 51 ◽  
pp. 1100-1101
Author(s):  
David A. Muller
Keyword(s):  
Thin Films ◽  
Electron Diffraction ◽  
Amorphous Carbon ◽  
Glassy Carbon ◽  
Spherical Structure ◽  
Local Ordering ◽  
Carbon Arc ◽  
Similar Appearance ◽  
Carbon Thin Films ◽  
Large Spherical

The sp2 rich amorphous carbons have a wide variety of microstructures ranging from flat sheetlike structures such as glassy carbon to highly curved materials having similar local ordering to the fullerenes. These differences are most apparent in the region of the graphite (0002) reflection of the energy filtered diffracted intensity obtained from these materials (Fig. 1). All these materials consist mainly of threefold coordinated atoms. This accounts for their similar appearance above 0.8 Å-1. The fullerene curves (b,c) show a string of peaks at distance scales corresponding to the packing of the large spherical and oblate molecules. The beam damaged C60 (c) shows an evolution to the sp2 amorphous carbons as the spherical structure is destroyed although the (220) reflection in fee fcc at 0.2 Å-1 does not disappear completely. This 0.2 Å-1 peak is present in the 1960 data of Kakinoki et. al. who grew films in a carbon arc under conditions similar to those needed to form fullerene rich soots.

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