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Journal articles on the topic 'Fullerene nanotube'

Author: Grafiati

Published: 28 May 2022

Last updated: 30 July 2025

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1

Morozova, E. V., and D. A. Timkaeva. "Effect of encapsulation of fullerene in semiconducting zigzagcarbon nanotubes on optical and thermoelectric properties." Journal of Physics: Conference Series 2086, no. 1 (2021): 012196. http://dx.doi.org/10.1088/1742-6596/2086/1/012196.

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Abstract We study the optical and thermoelectric properties of carbon nanotubes (CNTs) with encapsulated C60 fullerene molecules. Using ab-initio methods, we calculate optical and thermoelectric paramters for CNT with fullerenes periodically located inside the nanotube at different distances from each other. Dependencies of these parameters on fullerene concentration and diameter of CNT are analyzed.

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2

Farmanzade, Davood, and Leila Tabari. "Characterization of the fullerene end-functionalized ZnO nanotube: A computational study." Journal of Theoretical and Computational Chemistry 15, no. 04 (2016): 1650031. http://dx.doi.org/10.1142/s0219633616500310.

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The electronic and field emission properties of the fullerene end-functionalized zinc oxide nanotube (ZnONT) are investigated by density functional theory (DFT) to search for novel field emitter nano material. The interaction energies of ZnONT/fullerenes complexes gradually increase, with increasing the nanotube lengths which indicate that ZnONTs with higher lengths could improve the stability of the complexes. The band gaps of connected construction of fullerene molecules with ZnONTs gradually reduced by increasing the tube length, but were not sensitive to the tubes diameter. It is found tha

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3

Cox, Barry J., Ngamta Thamwattana, and James M. Hill. "Mechanics of atoms and fullerenes in single-walled carbon nanotubes. I. Acceptance and suction energies." Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences 463, no. 2078 (2006): 461–77. http://dx.doi.org/10.1098/rspa.2006.1771.

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Owing to their unusual properties, carbon nanostructures such as nanotubes and fullerenes have caused many new nanomechanical devices to be proposed. One such application is that of nanoscale oscillators which operate in the gigahertz range, the so-called gigahertz oscillators. Such devices have potential applications as ultrafast optical filters and nano-antennae. While there are difficulties in producing micromechanical oscillators which operate in the gigahertz range, molecular dynamical simulations indicate that nanoscale devices constructed of multi-walled carbon nanotubes or single-walle

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Cruz-Silva, Rodolfo, Takumi Araki, Takuya Hayashi, Humberto Terrones, Mauricio Terrones, and Morinobu Endo. "Fullerene and nanotube growth: new insights using first principles and molecular dynamics." Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences 374, no. 2076 (2016): 20150327. http://dx.doi.org/10.1098/rsta.2015.0327.

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Shortly after the discovery of fullerenes, many researchers pointed out that carbon nanotubes could be considered as elongated fullerenes. However, the detailed formation mechanism for both structures has been a topic of debate for several years, and consequently it has been difficult to draw a clear connection between the two systems. While the synthesis conditions appear to be different for both fullerenes and nanotubes, here, we demonstrate that it is highly likely that, at an initial growth stage, single-walled carbon nanotubes begin to grow from a hemisphere-like fullerene cap. More impor

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5

De Sousa, J. M., C. F. Woellner, L. D. Machado, P. A. S. Autreto, and D. S. Galvao. "Carbon Nanotube Peapods Under High-Strain Rate Conditions: A Molecular Dynamics Investigation." MRS Advances 5, no. 33-34 (2020): 1723–30. http://dx.doi.org/10.1557/adv.2020.139.

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ABSTRACTNew forms of carbon-based materials have received great attention, and the developed materials have found many applications in nanotechnology. Interesting novel carbon structures include the carbon peapods, which are comprised of fullerenes encapsulated within carbon nanotubes. Peapod-like nanostructures have been successfully synthesized, and have been used in optical modulation devices, transistors, solar cells, and in other devices. However, the mechanical properties of these structures are not completely elucidated. In this work, we investigated, using fully atomistic molecular dyn

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Levitsky, Semyon G., Vladislav V. Shunaev, and Olga E. Glukhova. "A Hybrid Nanocomposite Based on the T-Shaped Carbon Nanotubes and Fullerenes as a Prospect Material for Triple-Value Memory Cells." Materials 15, no. 22 (2022): 8175. http://dx.doi.org/10.3390/ma15228175.

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Relying on empirical and quantum chemical methods, a hybrid nanocomposite based on the T-shaped carbon nanotube (CNT) junction and internal fullerene C60 is proposed as a potential triple-value memory cell. The T-shaped CNT provides three potential wells where the internal fullerene can be located. The fullerene can move between these wells under the periodic external electric field, whose strength and frequency parameters are identified. The process of the fullerene’s motion control corresponds to the memory cell write operation. The read operation can be realized by determining the fullerene

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7

Cox, Barry J., Ngamta Thamwattana, and James M. Hill. "Mechanics of atoms and fullerenes in single-walled carbon nanotubes. II. Oscillatory behaviour." Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences 463, no. 2078 (2006): 477–94. http://dx.doi.org/10.1098/rspa.2006.1772.

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The discovery of carbon nanotubes and C 60 fullerenes has created an enormous impact on possible new nanomechanical devices. Owing to their unique mechanical and electronic properties, such as low weight, high strength, flexibility and thermal stability, carbon nanotubes and C 60 fullerenes are of considerable interest to researchers from many scientific areas. One aspect that has attracted much attention is the creation of high-frequency nanoscale oscillators, or the so-called gigahertz oscillators, for applications such as ultrafast optical filters and nano-antennae. While there are difficul

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8

Kovalchuk, O. V., I. P. Studenyak, T. M. Kovalchuk, et al. "Dielectric properties of Shell oil transformer oil with impurities of carbon nanotubes and fullerene C60." Semiconductor Physics, Quantum Electronics and Optoelectronics 24, no. 04 (2021): 413–18. http://dx.doi.org/10.15407/spqeo24.04.413.

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At the temperature 293 K, the influence of two types of nanoimpurities (carbon multiwall nanotubes and C60 fullerene) both separately and together on the dielectric properties of Shell oil transformer oil has been studied. It has been shown that these impurities do not significantly effect on the value of the dielectric permittivity of Shell oil, but more significantly increase its conductivity. It has been found that in the presence of nanotubes inside Shell oil, the dependence of its electrical conductivity on the fullerene concentration is nonmonotonic. The samples with the fullerene concen

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9

SLANINA, ZDENĚK, FILIP UHLÍK, LESZEK STOBINSKI, HONG-MING LIN, and LUDWIK ADAMOWICZ. "COMPUTING NARROW NANOTUBES AND THEIR DERIVATIVES." International Journal of Nanoscience 01, no. 03n04 (2002): 303–12. http://dx.doi.org/10.1142/s0219581x0200019x.

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Very recently, narrow nanotubes have been observed with diameters of 5 or even 4 Å. In this report we survey calculations that have so far been performed on narrow model nanotubes, namely capped by fragments of D2d and D6h C 36 fullerene cages or by fragments of C 32 and C 16quasi-fullerene cages with two four-membered rings, or finally by a fragment of dodecahedral C 20. The computations can reproduce the observed diameters of the narrow nanotubes. The results also indicate that fragments of C 32, used as caps instead of C 36, can lead to quite competitive energetics. Thus, a novel possibilit

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10

Kuzmany, Hans, Rudolf Pfeiffer, Martin Hulman, and Christian Kramberger. "Raman spectroscopy of fullerenes and fullerene–nanotube composites." Philosophical Transactions of the Royal Society of London. Series A: Mathematical, Physical and Engineering Sciences 362, no. 1824 (2004): 2375–406. http://dx.doi.org/10.1098/rsta.2004.1446.

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11

Koenig, Ryan M., and Steven Stevenson. "Selective Solubility of Fullertubes with Non-Aromatic Solvents." ECS Meeting Abstracts MA2022-01, no. 11 (2022): 835. http://dx.doi.org/10.1149/ma2022-0111835mtgabs.

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The recent experimental discovery of fullertubes has opened the door to fundamental studies in carbon nanomaterials. Fullertubes, comprised of half-fullerene end caps connected with a single-walled carbon nanotube belt, show evidence of the exciting properties of carbon nanotubes with the advantage of a defined, reproducible structure. However, large-scale quantities of these hybrid materials have yet to be realized due to their low abundance in electric arc extracts. Currently, fullertube isomers are isolated in two steps. In the first step, spheroidal fullerenes are reacted with aminopropano

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12

Noble, Cora A., and Steven Stevenson. "Detection and Isolation of Isomerically Pure C120 Fullertubes." ECS Meeting Abstracts MA2022-01, no. 11 (2022): 834. http://dx.doi.org/10.1149/ma2022-0111834mtgabs.

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The emergence of macroscopic amounts of C60 fullerenes and carbon nanotubes in the 1990s has led to an explosion of growth in new structures of carbon nanomaterials. Over the last decades, there have been theoretical predictions of a particular “hybrid” family of mathematical structures. Fullertubes represent a new area of fundamental research in molecular carbon. They are similar to fullerenes in structure, but with increasingly long cylindrical, single-wall nanotube belts in the middle of the molecules. These nanotube belts are similar to single-layer, rolled graphene. In 2020 we published t

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13

Kornyushin, Yuri. "Application of Thomas-Fermi model to fullerene molecule and nanotube." Facta universitatis - series: Physics, Chemistry and Technology 5, no. 1 (2007): 11–18. http://dx.doi.org/10.2298/fupct0701011k.

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Semiclassical description, based on electrostatics and Thomas-Fermi model is applied here to calculate dimensions of the electronic shell of a fullerene molecule and a nanotube. The internal radius of the electronic shell of a fullerene molecule, calculated within the framework of the model is 0.2808 nm. The external radius is 0.4182 nm. The experimental values are 0.279 nm and 0.429 nm correspondingly. This shows that semiclassical approach provides rather good description of the dimensions of the electronic shell in a fullerene molecule. Two types of dipole oscillations in a fullerene molecu

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14

Puente Santiago, Alain R. "Zero-Dimensional Carbon Nanomaterials: Building Blocks for Efficient Energy Conversion." Bionatura Journal 1, no. 3 (2024): 1–4. http://dx.doi.org/10.70099/bj/2024.03.01.1.

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Low-dimensional carbon-based materials, including 0D fullerene, 1D carbon nanotube, and 2D graphene, have been widely used as electroactive building blocks for sustainable energy conversion heterostructure nanosystems. These materials have unique physical and chemical properties at the nanoscale, such as high conductivity, high specific surface area, and tunable electronics, making them the focus of new renewable energy technologies. In this context, 0D carbon-based nanomaterials, like fullerenes and fullertubes, have garnered substantial attention as rising star energy materials. This editori

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15

Tanigaki, Katsumi. "Fullerene: C60 and Nanotube." Kobunshi 42, no. 6 (1993): 468–71. http://dx.doi.org/10.1295/kobunshi.42.468.

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16

Xie, Rui-Hua, and Qin Rao. "Third-order Optical Nonlinearities of Higher Fullerene and Carbon Nanotube." Zeitschrift für Naturforschung A 54, no. 10-11 (1999): 645–58. http://dx.doi.org/10.1515/zna-1999-10-1114.

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Recent theoretical and experimental studies on the third-order optical nonlinearities of higher fullerenes including C70, C76, C84, C86, C90, C94 and C96 are briefly reviewed. The extended Su-Schrieffer-Heeger model is introduced and applied to study the third-order optical nonlinearity of chiral carbon nanotubes (CCN), where the average contribution Γ of one carbon atom to the third-order optical nonlinearity of each CCN is calculated and compared with that of a well characterized polyenic polymer. It is found that (i) the smaller the diameter of a CCN, the larger the average contribution Γ;

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17

Bubenchikov, M., A. Bubenchikov, D. Mamontov, and V. Ovchinnikov. "Studying the possibility of using fullerenes inside carbon nanotubes as a molecular engine." Journal of Physics: Conference Series 2211, no. 1 (2022): 012005. http://dx.doi.org/10.1088/1742-6596/2211/1/012005.

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Abstract A simple model of a molecular engine is proposed, which consists of a fullerene dimer with a charge and a carbon nanotube. Calculations of molecular dynamics have been carried out, which help to estimate the efficiency of fullerene dimers as a molecular rotor. A dimer placed inside a carbon nanotube will move along the axis of the nanotube, but at the same time it needs to be given a lot of energy in order for it to leave it. The ability of molecules to move along a container is studied mechanically.

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18

Nature, Science. "Nanochip Medicine: Physical Chemistry Engineering." SCIENCE NATURE 2, no. 1 (2019): 086–89. http://dx.doi.org/10.30598/snvol2iss1pp086-089year2019.

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In providing the best nanocarbon-based medicine particularly associated with their multitasking healing system, an advanced knowledge and understanding of physical chemistry engineering is compulsory. Discovery of the first spherical nanocarbon cage C60, namely, fullerene or buckyball by R. Smalley and his colleague in ~1986 at Rice university made the former elected as a chemistry Nobel laureate 10 years later in 1996. Various investigations in conjunction with fullerenes had been tremendously pursued in many interesting research fields, especially, on its characters including nonlinear and o

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19

Ogloblya, O. V., D. Hui, Y. M. Strzhemechny, and Yu I. Prylutskyy. "Optical Polarizability of Zigzag Single-Walled Carbon Nanotubes Fullerene-Capped at One End and Covalently Bonded with Benzene Rings at the Other End." Journal of Nanomaterials 2007 (2007): 1–3. http://dx.doi.org/10.1155/2007/13617.

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We report on the results of numerical simulations for the linear optical polarizability of single-walled zigzag (9,0) carbon nanotubes with modified ends. The nanotubes of a variable length are fullerene-capped at one end and covalently bonded to a hydrophobic cluster of nine benzene rings at the other end. We investigate electronic and optical properties of such structures within a framework of the Su-Schrieffer-Heeger model. We demonstrated that the localized states in this system exhibit nonlinear characteristics of excited states. The nanotubes have a strongly oscillating dependence of the

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20

Stasyuk, Anton J., Olga A. Stasyuk, Miquel Solà, and Alexander A. Voityuk. "Photoinduced electron transfer in nanotube⊃C70 inclusion complexes: phenine vs. nanographene nanotubes." Chemical Communications 56, no. 83 (2020): 12624–27. http://dx.doi.org/10.1039/d0cc04261g.

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The six-atom vacancy defects regularly located throughout the nanotubes change the electronic properties of their inclusion complexes with fullerene and prevent the photoinduced electron transfer between host and guest molecules.

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21

Li, Chang Sheng, Ke Hong Yan, Jun Mao Li, Xiao Ping Shen, and Kang Min Chen. "Investigation of Micro-Tribological Behavior of MS₂ Nanotubes." Solid State Phenomena 121-123 (March 2007): 785–88. http://dx.doi.org/10.4028/www.scientific.net/ssp.121-123.785.

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It is well known that metal dichalcogenides MS2 (M=Mo, W, Nb, Ta, TiS, Zr ,Hf, S=S, Se) have lamellar structure, the bonds of adjacent lamellae are weak van der Waals interactions and inter-lamellar are strong covalent interactions. The structures make adjacent lamellae easy to slip and it shows low friction coefficient during friction process. MS2 are often used as solid lubricants in high/low temperature, heave load and vacuum, in which oil is failure. WS2 has better high temperature properties than MoS2, although little natural WS2 mineral has been deposited, and people must synthesize it b

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22

Amusia, M. Ya, and A. S. Baltenkov. "Elastic scattering of slow electrons by carbon nanotubes." Journal of Physics B: Atomic, Molecular and Optical Physics 54, no. 24 (2021): 245201. http://dx.doi.org/10.1088/1361-6455/ac3c94.

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Abstract In this paper we calculate the cross sections for elastic scattering of slow electrons by carbon nanotubes. The corresponding electron–nanotube interaction is substituted by a zero-thickness cylindrical potential that neglects the atomic structure of real nanotubes, thus limiting the range of applicability of our approach to sufficiently low incoming electron energies. The strength of the potential is chosen to be the same as was used in describing the scattering of electrons by fullerene C60. We present results for total and partial electron scattering cross sections as well as their

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23

Urolov, Ikrom Z., Farid F. Umarov, Ishmumin D. Yadgarov, Ganiboy T. Rakhmanov, and Khayitmurod I. Jabborov. "Computer Simulation of Adsorption of C60 Fullerene Molecule on Reconstructed Si(100) Surface." East European Journal of Physics, no. 2 (June 1, 2024): 256–62. http://dx.doi.org/10.26565/2312-4334-2024-2-25.

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The adsorption of the C60 fullerene molecule has been studied in various configurations on a reconstructed Si(100) silicon surface. Among fullerenes, fullerene C60 is of particular importance since it has the most stable form and consists of 60 carbon atoms. Monocrystalline silicon has the diamond structure, the size of its crystal lattice is 5.43 Å. The MD-simulation calculations have been performed using the open source LAMMPS MD-simulator software package and the Nanotube Modeler computer program. The Tersoff interatomic potential has been used to determine the interactions between the Si-S

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24

UDOMVECH, ANURAK, TEERAKIAT KERDCHAROEN, VUDHICHAI PARASUK, YUTHANA TANTIRUNGROTECHAI, and TANAKORN OSOTCHAN. "ELECTRONIC STRUCTURE OF THE FINITE-SIZED SINGLE-WALLED CARBON NANOTUBES." International Journal of Nanoscience 02, no. 03 (2003): 141–52. http://dx.doi.org/10.1142/s0219581x03001176.

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The effects of tubule length and terminal capping on the geometrical and electronic properties of finite-sized zig-zag (9, 0) single-walled carbon nanotubes (SWNT), which length varying from 2 up to 12 unit cells (~50 Å), were investigated using molecular mechanics, semi-empirical methods (AM1 and EHMO) and density functional theory (B3LYP). AM1 method indicates how the nanotube ends are capped affects strongly the tubule geometric parameters. Although these effects seem to decrease exponentially as the tube gets longer, the converging values for C–C bond length in the open- and closed-end str

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25

Yang, Xueming, Longjie Wang, Yanhui Huang, Zhonghe Han, and Albert C. To. "Carbon nanotube–fullerene hybrid nanostructures by C60 bombardment: formation and mechanical behavior." Phys. Chem. Chem. Phys. 16, no. 39 (2014): 21615–19. http://dx.doi.org/10.1039/c4cp02620a.

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26

Gumbs, Godfrey, Antonios Balassis, Andrii Iurov, and Paula Fekete. "Strongly Localized Image States of Spherical Graphitic Particles." Scientific World Journal 2014 (2014): 1–6. http://dx.doi.org/10.1155/2014/726303.

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We investigate the localization of charged particles by the image potential of spherical shells, such as fullerene buckyballs. These spherical image states exist within surface potentials formed by the competition between the attractive image potential and the repulsive centripetal force arising from the angular motion. The image potential has a power law rather than a logarithmic behavior. This leads to fundamental differences in the nature of the effective potential for the two geometries. Our calculations have shown that the captured charge is more strongly localized closest to the surface

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27

Wang, Yan, Mingguang Yao, Xing Hua, et al. "Structural Evolution of D _5h(1)-C₉₀ under High Pressure: A Mediate Allotrope of Nanocarbon from Zero-Dimensional Fullerene to One-Dimensional Nanotube." Chinese Physics Letters 39, no. 5 (2022): 056101. http://dx.doi.org/10.1088/0256-307x/39/5/056101.

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The hybridization of fullerene and nanotube structures in newly isolated C90 with the D 5h symmetric group (D 5h (1)-C90) provides an ideal model as a mediating allotrope of nanocarbon from zero-dimensional (0D) fullerene to one-dimensional nanotube. Raman and infrared spectroscopy combined with classical molecular dynamics simulation were used to investigate the structural evolution of D 5h (1)-C90 at ambient and high pressure up to 35.1 GPa. Interestingly, the high-pressure transformations of D 5h (1)-C90 exhibit the features of both fullerene and nanotube. At around 2.5 GPa, the D 5h (1)-C9

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28

Gonzalez Carmona, Juan Manuel, Alexander Ruden Muñoz, Christian Barbosa, Carolina Ortega Portilla, and Federico Sequeda Osorio. "Computational Study of Allotropic Structures of Carbon by Density Functional Theory (DTF)." Ingeniería y Ciencia 10, no. 19 (2014): 145–62. http://dx.doi.org/10.17230/ingciencia.10.19.7.

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In this paper using Density Functional Theory (DFT), the principal carbonallo tropic crystalline structures (Diamond, graphite, nanotube y fullerene-C60) were simulated. The results shows diamond sp3 bonds formation between carbon atomsand low reactivity, indicating low probability of lateral compound formation and high mechanical properties. Interplanar weakness was evidentin graphite structure, which is related to solid lubrication process. Carbon-Carbon metallic bonds and polarizations at the edges of the structure were observed in Armchair Carbon Nanotube, stabilizing the system which allo

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29

Bourret, Emmanuel, Michel Côté, and Steven Stevenson. "(Invited) Anisotropic Contributions in the Chromatographic Elution Behavior of Fullerenes and Fullertubes." ECS Meeting Abstracts MA2023-01, no. 12 (2023): 1260. http://dx.doi.org/10.1149/ma2023-01121260mtgabs.

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Since their discovery in the mid-1980s, the fullerenes have been confined to molecules of less than 100 atoms. With the recent development of a method allowing the isolation of pristine samples[1], the discovery of increasingly long fullertubes, hybrid between a fullerene and a nanotube, is stimulating renewed interest in the field of fullerene science. The increase in the number of atoms comes at a price, the explosion in the number of possible isomers, among which we must identify the experimentally isolated structure. Fuch’s model[2] is commonly used to explain the interaction between fulle

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Kobeleva, Elena S., Mikhail N. Uvarov, Natalia V. Kravets, et al. "Ternary Composite of Polymer, Fullerene and Fluorinated Multi-Walled Carbon Nanotubes as the Active Layer of Organic Solar Cells." Journal of Composites Science 8, no. 1 (2023): 3. http://dx.doi.org/10.3390/jcs8010003.

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Fluorinated multi-walled carbon nanotubes are implemented as the third component of the active layer of organic solar cells. The addition of approximately 1% weight fraction of these nanotubes into PCDTBT/PC60BM polymer/fullerene active layer leads to a noticeable increase in the main photovoltaic parameters of the solar cells, including their stability. Presumably, the origins of this influence are optimizing the donor/acceptor composite morphology and reinforcing its structure with fluorinated multi-walled carbon nanotubes. This hypothesis is supported by the dramatic influence of the fluori

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31

Turabekova, M., B. Rasulev, M. Theodore, J. Jackman, D. Leszczynska, and J. Leszczynski. "Immunotoxicity of nanoparticles: a computational study suggests that CNTs and C60 fullerenes might be recognized as pathogens by Toll-like receptors." Nanoscale 6, no. 7 (2014): 3488–95. http://dx.doi.org/10.1039/c3nr05772k.

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Guillard, Tony, Gilles Flamant, Jean-Franc¸ois Robert, Bruno Rivoire, Joseph Giral, and Daniel Laplaze. "Scale up of a Solar Reactor for Fullerene and Nanotube Synthesis." Journal of Solar Energy Engineering 124, no. 1 (2001): 22–27. http://dx.doi.org/10.1115/1.1434263.

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Conventional methods for the synthesis of fullerenes and carbon nanotubes such as laser or electric arc ablation have failed when the process is scaled up. Our ultimate goal is to scale a solar process up from 2 to 250 kW; this paper shows that our method for achieving this scale-up is valid because we were able to predict process performance variables at the 50 kW level from preliminary experimental results from 2 kW experiments. The key parameters that characterize this process are the carbon soot mass flow rate and the desired product yield. The carbon soot production rate is a function of

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33

Abbood et al., Amal. "Synthesis of C60 Nanotube from Pyrolysis of Plastic Waste (Polypropylene) with Catalyst." Baghdad Science Journal 17, no. 2(SI) (2020): 0624. http://dx.doi.org/10.21123/bsj.2020.17.2(si).0624.

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Fullerene nanotube was synthesized in this research by pyrolysis of plastic waste Polypropylene (PP) at 1000 ° C for two hours in a closed reactor made from stainless steel using molybdenum oxide (MoO3) as a catalyst and nitrogen gas. The resultant carbon was purified and characterized by energy dispersive X-ray spectroscopy (EDX), X-ray powder diffraction (XRD). The surface characteristics of C60 nanotubes were observed with the Field emission scanning electron microscopy (FESEM). The carbon is evenly spread and has the highest concentration from SEM-EDX characterization. The result of XRD an

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34

Xu, Zong Wei, Feng Zhou Fang, and Xiao Tang Hu. "Fabrication of Carbon Nanotube Probes in Atomic Force Microscopy." Advanced Materials Research 76-78 (June 2009): 497–501. http://dx.doi.org/10.4028/www.scientific.net/amr.76-78.497.

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Carbon nanotube (CNT) probe used in atomic force microscopy (AFM) was fabricated by using electron beam induced Pt deposition method. The bonding force for CNT probe was found to be larger than 500nN. The nanotube probe’s length was shortened by focused ion beam milling process. It is confirmed that the CNT probe shows higher aspect ratio than the Si probe. The nanotube probes with fullerene-like cap end present higher imaging resolution than those with open end.

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SHEN, HAIJUN. "TENSILE PROPERTIES AND ELECTRONIC STRUCTURES OF C240 NANOTUBE AND 4C60 FULLERENE POLYMERS." International Journal of Nanoscience 05, no. 01 (2006): 99–107. http://dx.doi.org/10.1142/s0219581x06004073.

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The classical MD (Molecular Dynamics) method was used to simulate the tension of three kinds of C 240 isomers, i.e., C 240 nanotube, chain-like 4C 60 fullerene polymer and peanut-like 4C 60 fullerene polymer. Then, the semi-empirical PM3 method was used to calculate their electronic structures under tension. Lastly, according to the calculated results, their differences in tensile mechanical properties, as well as the change of their FMO (Frontier Molecular Orbital) energy during tension, were discussed. It is shown that: (1) the load-support capability of the C 240 molecules has the order of

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PACHOS, JIANNIS K., and MICHAEL STONE. "AN INDEX THEOREM FOR GRAPHENE." International Journal of Modern Physics B 21, no. 30 (2007): 5113–20. http://dx.doi.org/10.1142/s0217979207038228.

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We consider a graphene sheet folded in an arbitrary geometry, compact or with nanotube-like open boundaries. In the continuous limit, the Hamiltonian takes the form of the Dirac operator, which provides a good description of the low energy spectrum of the lattice system. We derive an index theorem that relates the zero energy modes of the graphene sheet with the topology of the lattice. The result coincides with analytical and numerical studies for the known cases of fullerene molecules and carbon nanotubes, and it extends to more complicated molecules. Potential applications to topological qu

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Gong, Maogang, Tejas A. Shastry, Yu Xie, et al. "Polychiral Semiconducting Carbon Nanotube–Fullerene Solar Cells." Nano Letters 14, no. 9 (2014): 5308–14. http://dx.doi.org/10.1021/nl5027452.

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Byszewski, Przemysław, Hubert Lange, Andrzej Huczko, and Jürgen F. Behnke. "Fullerene and nanotube synthesis. plasma spectroscopy studies." Journal of Physics and Chemistry of Solids 58, no. 11 (1997): 1679–83. http://dx.doi.org/10.1016/s0022-3697(97)00051-6.

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Hodak, Miroslav, and L. A. Girifalco. "Cohesive properties of fullerene-filled nanotube ropes." Chemical Physics Letters 363, no. 1-2 (2002): 93–98. http://dx.doi.org/10.1016/s0009-2614(02)01098-9.

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Wang, Changchun, Zhi-Xin Guo, Shoukuan Fu, Wei Wu, and Daoben Zhu. "Polymers containing fullerene or carbon nanotube structures." Progress in Polymer Science 29, no. 11 (2004): 1079–141. http://dx.doi.org/10.1016/j.progpolymsci.2004.08.001.

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Tiangtrong, Prangsai, and Narong Chaihathep. "The New Design Nanocapsules from Interactions between Atoms and Carbon Nanotubes with End Caps." Journal of Nanomaterials 2021 (October 8, 2021): 1–9. http://dx.doi.org/10.1155/2021/9997880.

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A massive interest has arisen in nanocapsule, and it is used in different fields. Carbon nanotubes and fullerene are the most commonly used nanomaterials due to their remarkable properties, such as optical, mechanical, electrical, and thermal properties. Especially in biomedical science, nanocapsules are highly recommended to be applied as carriers for drugs. From the Magic bullet theory, it is expected that the nanocapsules can deliver drugs to the target cells, which can reduce the side effects on the nontargeted cells. In this research, we design a new nanocapsule consisting of a finite-len

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Choi, Ji Il, Hyo Seok Kim, Han Seul Kim, Ga In Lee, Jeung Ku Kang, and Yong-Hoon Kim. "Carbon nanobuds based on carbon nanotube caps: a first-principles study." Nanoscale 8, no. 4 (2016): 2343–49. http://dx.doi.org/10.1039/c5nr07188g.

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The formation of fullerene carbon nanobuds (CNBs) on carbon nanotube (CNT) caps is energetically more favorable than that on CNT sidewalls. Generally, CNBs based on CNT ends can induce resonant transmissions near the Fermi level.

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Abdulnabi, Hussein A., and Yasin Yousif Al-Aboosi. "Design of Tunable Multiband Hybrid Graphene Metal Antenna in Microwave Regime." Indonesian Journal of Electrical Engineering and Computer Science 12, no. 3 (2018): 1003. http://dx.doi.org/10.11591/ijeecs.v12.i3.pp1003-1009.

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<p>Graphene is an <a title="Allotrope" href="https://en.wikipedia.org/wiki/Allotrope">allotrope</a> (form) of carbon consisting of a single layer of carbon atoms arranged in an <a title="Hexagonal lattice" href="https://en.wikipedia.org/wiki/Hexagonal_lattice">hexagonal lattice</a>. It is the basic structural element of many other allotropes of carbon, such as <a title="Graphite" href="https://en.wikipedia.org/wiki/Graphite">graphite</a>, <a title="Charcoal" href="https://en.wikipedia.org/wiki/Charcoal">charcoal</a>, <a title="Carbon nan

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Jia, Guang, Haifang Wang, Lei Yan, et al. "Cytotoxicity of Carbon Nanomaterials: Single-Wall Nanotube, Multi-Wall Nanotube, and Fullerene." Environmental Science & Technology 39, no. 5 (2005): 1378–83. http://dx.doi.org/10.1021/es048729l.

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Pallasser, Robert, Louis S. K. Pang, Luke Prochazka, Donald Rigby, and Michael A. Wilson. "Isotopic fractionation during fullerene, nanotube, and nanopolyhedra formation." Journal of the American Chemical Society 115, no. 24 (1993): 11634–35. http://dx.doi.org/10.1021/ja00077a087.

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Uberuaga, Blas P., Steven J. Stuart, Wolfgang Windl, Michael P. Masquelier, and Arthur F. Voter. "Fullerene and graphene formation from carbon nanotube fragments." Computational and Theoretical Chemistry 987 (May 2012): 115–21. http://dx.doi.org/10.1016/j.comptc.2011.11.030.

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Zhao, Jijun, Bin Wen, Zhen Zhou, et al. "Novel Carbon Nanotube Peapods Encapsulating Au32 Golden Fullerene." Journal of Computational and Theoretical Nanoscience 3, no. 3 (2006): 459–62. http://dx.doi.org/10.1166/jctn.2006.3030.

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Umeyama, Tomokazu, Jinseok Baek, Noriyasu Tezuka, Kazuki Morita, and Hiroshi Imahori. "Incorporation of Graphene to Fullerene Clusters and Fullerene-Nanotube Composites and Their Photoelectrochemical Properties." ECS Journal of Solid State Science and Technology 2, no. 10 (2013): M3001—M3007. http://dx.doi.org/10.1149/2.001310jss.

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Armaghani, Sahar, Ali Rostami, and Peyman Mirtaheri. "Graphene Nanoribbon Bending (Nanotubes): Interaction Force between QDs and Graphene." Coatings 12, no. 9 (2022): 1341. http://dx.doi.org/10.3390/coatings12091341.

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Carbon materials in different shapes—such as fullerene molecules (0D), nanotubes and graphene nanoribbons (1D), graphene sheets (2D), and nanodiamonds (3D)—each have distinct electrical and optical properties. All graphene-based nanostructures are expected to exhibit extraordinary electronic, thermal, and mechanical properties. Moreover, they are therefore promising candidates for a wide range of nanoscience and nanotechnology applications. In this work, we theoretically studied and analyzed how an array of quantum dots affects a charged graphene plate. To that end, the array of quantum dots w

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Skupov, Kirill, and Alex Adronov. "Effect of carbon nanotube incorporation into polythiophene-fullerene-based organic solar cells." Canadian Journal of Chemistry 92, no. 1 (2014): 68–75. http://dx.doi.org/10.1139/cjc-2013-0460.

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The effect of single-walled carbon nanotube (SWNT) incorporation within bulk heterojunction photovoltaic devices based on poly(3-hexylthiophene) − [6,6]-phenyl-C61-butyric acid methyl ester (P3HT−PCBM) (1:1 w/w) active layers was investigated. Both full-length and shortened SWNTs were introduced within the P3HT−PCBM layer at loadings in the range of 0−2 wt%. For full-length SWNTs, it was found that device efficiency decreased at all SWNT loading levels and annealing temperatures, which ranged from 80 to 225 °C. The highest average external efficiencies in the absence of SWNTs reached approxima

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