Ivaylo Hinkov

Mr. Ivaylo Hinkov

orcid

Research Focus & Metrics

Academic Career Length

23Years (2004-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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24 June 2005 in Carbon
Verified
Journal Article
Closed access
IHIvaylo Hinkov
Ivaylo Hinkov
SFS. Farhat
S. Farhat
CSC.D. Scott
C.D. Scott

1 September 2016 in Materials Today Communications
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Journal Article
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ABAbir Ben Belgacem
Abir Ben Belgacem
IHIvaylo Hinkov
Ivaylo Hinkov
SYSana Ben Yahia
Sana Ben Yahia
OBOvidiu Brinza
Ovidiu Brinza
SFSamir Farhat
Samir Farhat

15 February 2004 in Journal of Applied Physics
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Journal Article
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IHIvaylo Hinkov
Ivaylo Hinkov
JGJ. Grand
J. Grand
MCM. Lamy de la Chapelle
M. Lamy de la Chapelle
SFS. Farhat
S. Farhat
CSC. D. Scott
C. D. Scott
SLS. Lefrant
S. Lefrant
The diameter distribution of the nanotubes produced by electric-arc discharge are measured using Raman spectroscopy at various wavelengths. These measurements agree with the results provided by two other techniques: high-resolution transmission electron microscopy and x-ray diffraction. The mean tube diameter shifts more than 0.1 nm with the increase of argon in the inert atmosphere. Some argon concentrations favored the synthesis of metallic tubes with specific diameters. Furthermore, the background gas influences the macroscopic characteristics of nanotube yield and bundle size, as determined by Brunauer–Emmett–Teller surface area measurements and x-ray diffraction. The information collected on nanotube diameter and arrangement is correlated with temperatures calculated using a numerical model of the plasma generated between the two electrodes. Indeed, plasma temperature control during the production process is achieved using argon–helium mixtures as buffer gases. The variation of the gas mixture from pure argon to pure helium changes the plasma temperature and hence the nanotube diameter.

1 April 2019 in Plasma Sources Science and Technology
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Journal Article
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KPKatya Pashova
Katya Pashova
IHIvaylo Hinkov
Ivaylo Hinkov
XAXavier Aubert
Xavier Aubert
SPSwaminathan Prasanna
Swaminathan Prasanna
Fabien BénédicFabien Bénédic
Fabien Bénédic
SFSamir Farhat
Samir Farhat
In this article, we report on some of the fundamental chemical and physical processes responsible for the deposition of graphene by microwave plasma-enhanced chemical vapor deposition. The graphene is grown by plasma decomposition of a methane and hydrogen mixture (CH 4 /H 2 ) at moderate pressures over polycrystalline metal catalysts. Different conditions obtained by varying the plasma power (300–400 W), total pressure (10–25 mbar), substrate temperature (700 °C–1000 °C), methane flow rate (1–10 sccm) and catalyst nature (Co–Cu) were experimentally analyzed using the in situ optical emission spectroscopy technique to assess the species rotational temperature of the plasma and the H-atom relative concentration. Then, two modeling approaches were developed to analyze the plasma environment during graphene growth. As a first approximation, the plasma is described by spatially averaged bulk properties, and the species compositions are determined using kinetic rates in the transient zero-dimensional (0D) configuration. The advantage of this approach lies in its small computational demands, which enable rapid evaluation of the effects of reactor conditions and permit the identification of dominant reactions and key species during graphene growth. This approach is useful for identifying the relevant set of species and reactions to consider in a higher-dimensional model. The reduced chemical scheme was then used within the self-consistent two-dimensional model (2D) to determine auto-coherently the electromagnetic field, gas and electron temperatures, heavy species, and electron and ion density distributions in the reactor. The 0D and 2D models are validated by comparison with experimental data obtained from atomic and molecular emission spectra.

17 January 2015 in AIChE Journal
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Journal Article
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MHMongia Hosni
Mongia Hosni
FSFARHAT Samir
FARHAT Samir
MAMounir Ben Amar
Mounir Ben Amar
AKAndrei Kanaev
Andrei Kanaev
NJNoureddine Jouini
Noureddine Jouini
IHIvaylo Hinkov
Ivaylo Hinkov

25 March 2020 in Coatings
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Journal Article
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KAKane Aichata
Kane Aichata
IHIvaylo Hinkov
Ivaylo Hinkov
OBOvidiu Brinza
Ovidiu Brinza
MHMongia Hosni
Mongia Hosni
ABAliou Hamady Barry
Aliou Hamady Barry
SFSamir Farhat
Samir Farhat
In this paper, we report on a modified arc process to synthetize graphene, copper and zinc oxide graphene hybrids. The anode was made of pure graphite or graphite mixed with metals or metal oxides. After applying a controlled direct current, plasma is created in the interelectrode region and the anode is consumed by eroding. Continuous and abundant flux of small carbon, zinc or copper species, issued from the anode at a relatively high temperature, flows through the plasma and condenses in the vicinity of a water-cooled cathode leading to few-layered graphene sheets and highly ordered carbon structures. When the graphite rod is filled with copper or zinc oxide nanoparticles, few layers of curved graphene films were anchored with spherical Cu and ZnO nanoparticles leading to a one-step process synthesis of graphene hybrids, which combine the synergetic properties of graphene along with nanostructured metals or semiconducting materials. The as-prepared samples were characterized by Raman spectroscopy, X-ray diffraction (XRD), spatially resolved electron energy loss spectroscopy (EELS), energy filtered elemental mapping and transmission electron microscopy (TEM). In addition to the experimental study, numerical simulations were performed to determine the velocity, temperature and chemical species distributions in the arc plasma under specific graphene synthesis conditions, thereby providing valuable insight into growth mechanisms.