Transparent, superhard amorphous carbon phase from compressing glassy carbon

2014 ◽  
Vol 104 (2) ◽  
pp. 021916 ◽  
Author(s):  
Mingguang Yao ◽  
Junping Xiao ◽  
Xianhong Fan ◽  
Ran Liu ◽  
Bingbing Liu
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.


2020 ◽  
Vol 860 ◽  
pp. 190-195
Author(s):  
Irma Septi Ardiani ◽  
Khoirotun Nadiyyah ◽  
Anna Zakiyatul Laila ◽  
Sarayut Tunmee ◽  
Hideki Nakajima ◽  
...  

Amorphous carbon films have been explored and used in a wide variety of applications. With the n-type and p-type amorphous carbon film, it can be used to make p-n junctions for solar cells. This research aims to study the structure of boron- and nitrogen-doped amorphous carbon (a-C:B and a-C:N) films. This research uses the basic material of bio-product from palmyra sugar to form amorphous carbon. Amorphous carbon was synthesized by heating the palmyra sugar at 250°C. The results of XRD showed that the doped films produce an amorphous carbon phase. PES was used to analyze the bonding state of dopants in the sample. B4C, BC3, and BC2O bonds formed in a-C:B, while pyridine and pyrrolic formed in a-C:N.


2016 ◽  
Vol 881 ◽  
pp. 441-446
Author(s):  
Graciele Vieira Barbosa ◽  
Igor Silva de Sá ◽  
Eliane Kujat Fischer ◽  
Tiziana Azario de Medeiros ◽  
Margarete Soares da Silva ◽  
...  

Nickel-silica nanocomposites can be obtained by direct chemical route, such as the Polymeric Precursor Method. That methodology type permits to obtain material powders with significant specific area and porosity suitable for reactive gases or fluids permeation, which are required characteristics for application in heterogeneous catalysis process. The composite material obtained from pyrolysis of polymeric precursor has its porosity strongly dependent from precursor constitution, which affects the decomposition kinetic. In this study, it was obtained a polyester precursor based on triethylene glycol, which has been submitted at pyrolysis at 600 oC for several times in nitrogen atmosphere. The nickel-silica nanocomposite obtained through that methodology presents a residual amorphous carbon phase playing an important rule on the mechanism of pore formation. Nickel nanoparticles nucleate with sizes close to 10 nm in diameter and are highly dispersed in a hybrid amorphous carbon-silica matrix. The composite pore volume, calculated through the JBH method, presents a continuous increasing as a function of pyrolysis time, reaching more than 0.15 cc/g after 7 hours from initial decomposition process.


2000 ◽  
Vol 14 (02n03) ◽  
pp. 113-124 ◽  
Author(s):  
S. LOGOTHETIDIS

Amorphous carbon (a-C) films, single and multilayered, were deposited by rf magnetron sputtering, from graphite, on c-Si substrates. In-situ and real-time Spectroscopic Ellipsometry (SE) was used to determine the optimum deposition conditions where the formation of controllable sp 3 sties can be achieved. The growth mechanisms of sputtered a-C films and their properties (optical, compositional, density and mechanical) were studied using a variety of novel characterization techniques. SE data analysis provides: (i) the sp 3 and sp 2 volume fractions and (ii) the optical properties, that are combined well with the density, the internal stresses and the elastic properties of ultra-thin to thick a-C films. In sputtering, the applied substrate bais voltage Vb (up to -200V) controls the energy (30≤E≤230 eV) of the Ar+ ions bombarding the growing film surface, affecting all film properties and responses and classifying the films in three types. The film developed with E≈30 eV (rich in sp 2 sites) and 30<E≤130 eV (rich in sp 3 sites) are defined by type I and II, respectively. Type III is defined by films developed with E>130 eV, where the formation of a new and dense carbon phase is deteched, exhibiting a semi-metallic optical behavior. The experimental results show: a) in films of type I and II the stress, density, hardness and elastic modulus are directly related with the sp 3 content and described well with the so far proposed models on the formation mechanism of tetrahedral carbon, and b) the density and the elastic properties, in type III films, depend not only on the sp 3 content but also on the new carbon phase. a-C films deposited by sputtering exhibit unique properties that can be tailored to meet specific application requirements. For example, the combination of single a-C films of type I and II in developing multilayered films resulted to the growth of stable, thick and highly sp 3 bonded films with improved elastic properties.


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