Porosity of Nanostructured Carbon Thin Films

Author(s):  
Alessandra Del Giudice ◽  
Giulio Benetti ◽  
Claudio Piazzoni ◽  
Francesca Borghi
2012 ◽  
Vol 7 (1) ◽  
pp. 286 ◽  
Author(s):  
Maziar Shakerzadeh ◽  
Edwin Hang Tong Teo ◽  
Beng Kang Tay

2001 ◽  
Vol 10 (3-7) ◽  
pp. 1195-1200 ◽  
Author(s):  
C Lenardi ◽  
E Barborini ◽  
V Briois ◽  
L Lucarelli ◽  
P Piseri ◽  
...  

2011 ◽  
Vol 509 (5) ◽  
pp. 1418-1423 ◽  
Author(s):  
D.B. Mahadik ◽  
S.S. Shinde ◽  
C.H. Bhosale ◽  
K.Y. Rajpure

Author(s):  
J. Kulik ◽  
Y. Lifshitz ◽  
G.D. Lempert ◽  
S. Rotter ◽  
J.W. Rabalais ◽  
...  

Carbon thin films with diamond-like properties have generated significant interest in condensed matter science in recent years. Their extreme hardness combined with insulating electronic characteristics and high thermal conductivity make them attractive for a variety of uses including abrasion resistant coatings and applications in electronic devices. Understanding the growth and structure of such films is therefore of technological interest as well as a goal of basic physics and chemistry research. Recent investigations have demonstrated the usefulness of energetic ion beam deposition in the preparation of such films. We have begun an electron microscopy investigation into the microstructure and electron energy loss spectra of diamond like carbon thin films prepared by energetic ion beam deposition.The carbon films were deposited using the MEIRA ion beam facility at the Soreq Nuclear Research Center in Yavne, Israel. Mass selected C+ beams in the range 50 to 300 eV were directed onto Si {100} which had been etched with HF prior to deposition.


Author(s):  
David A. Muller

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.


2013 ◽  
Vol 133 (5) ◽  
pp. 293-299
Author(s):  
Kiyotoshi Fujii ◽  
Etsuo Fujiwara ◽  
Masayoshi Shimizu ◽  
Shozo Inoue

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