Nanoscience and Nanotechnology
p-ISSN: 22163-257X e-ISSN: 2163-2588
2012; 2(4): 116-124
doi: 10.5923/j.nn.20120204.05
Aleksandr Eletskii 1, 2, Adilbek Erkimbaev 2, Georgy Kobzev 2, Michael Trachtengerts 2, Vladimir Zitserman 2
1Russian Research Centre “Kurchatov Institute”, Moscow, Russian Federation
2Joint Institute for High Temperatures, Russian Academy of Sciences, Izhorskaya 13, Bldg. 2, Moscow 125412, Russin Federation
Correspondence to: Vladimir Zitserman , Joint Institute for High Temperatures, Russian Academy of Sciences, Izhorskaya 13, Bldg. 2, Moscow 125412, Russin Federation.
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Copyright © 2012 Scientific & Academic Publishing. All Rights Reserved.
This paper reviews general problems appearing in collecting, categorization, and certification of numerical properties data for nanoscale objects. It is shown how their peculiar physical properties affect preparation of the data at the preliminary stage before moving to detailed data base design. As an example, the properties data of carbon nanoforms (nanotubes, graphene, etc) are presented. The key features of the nanosized data are revealed, such as: permanent variations of the properties nomenclature, dimensional effect, and high level of the data uncertainty. The procedure is proposed for data certification taking into account quantitative statement of uncertainty as well as quality indicators. The former present the completeness of the description both of an object and a method as well the result reproducibility.
Keywords: Nanostructure, Nanomaterial, Numeric Properties Data, Dimensional Effect, Logical Structure Semistructured Data, Data Certification
 of space between grains, and so forth[15], may affect appreciably physical properties. Such supplementary data are also necessary for valid specification a nanomaterial, along with description of the material origin and its processing history. For example, full details are ultimately necessary for carbon cloth-like materials made with single-wall CNT, multilayered graphene paper, CNT yarn, etc.It is necessary to bear in mind that both geometrical and physical parameters of nanoscale units can show variations in values. Distribution of these parameters depends on methods and conditions in production and noticeably affects the numeric properties data. An example[16] demonstrates importance of detailed description. Processing of single-walled CNT film by nitric acid changes the type of electrical conductivity from semi-conductor to metallic[17]. Such processing removes attached molecules or absorbed radicals from surface of CNT that changes dramatically the electronic structure of an object.The above example demonstrates once more that there are some other factors which have influence on data uncertainty ― in particular molecules or radicals absorbed on surface. The physical properties of such objects are determined by a relatively large contribution of the surface as compared to bulk. Radicals’ adsorption by the CNT or graphene surface is responsible for the variation of electronic structure that has an immediate impact on electrical properties. Thus, electrical conductivity of pure graphene sheet is 100-1000 times larger than that of partially oxidated graphene with 10 % of oxygen[18]. It is caused by the energy gap that occurs at graphene oxidation. Thermal conductivity of graphene also decreases as the number of the absorbed radicals increases. The absorbed radicals act as the scattering centers for phonons, hindering collisionless movement along the specimen. There are some processes that remove radicals by heat or chemical treatment. To sum up, reliable data on type and amount of adsorbed radicals are necessary in addition to geometry and object structure characteristics for unambiguous characterization of the object as well as for data evaluation. Hence, the measured properties of nanoobjects have unremovable uncertainty that stems from their atomic structure. Nevertheless, needs of engineering design or scientific research demand, that the property data have a certain certification of quality or an integrated estimation of uncertainty. This estimation should be based on accessible data on size and structure of object, method of measurement, method of synthesis, etc. Some more details are considered in section 6.
 of space between grains, and so forth[15], may affect appreciably physical properties. Such supplementary data are also necessary for valid specification a nanomaterial, along with description of the material origin and its processing history. For example, full details are ultimately necessary for carbon cloth-like materials made with single-wall CNT, multilayered graphene paper, CNT yarn, etc.It is necessary to bear in mind that both geometrical and physical parameters of nanoscale units can show variations in values. Distribution of these parameters depends on methods and conditions in production and noticeably affects the numeric properties data. An example[16] demonstrates importance of detailed description. Processing of single-walled CNT film by nitric acid changes the type of electrical conductivity from semi-conductor to metallic[17]. Such processing removes attached molecules or absorbed radicals from surface of CNT that changes dramatically the electronic structure of an object.The above example demonstrates once more that there are some other factors which have influence on data uncertainty ― in particular molecules or radicals absorbed on surface. The physical properties of such objects are determined by a relatively large contribution of the surface as compared to bulk. Radicals’ adsorption by the CNT or graphene surface is responsible for the variation of electronic structure that has an immediate impact on electrical properties. Thus, electrical conductivity of pure graphene sheet is 100-1000 times larger than that of partially oxidated graphene with 10 % of oxygen[18]. It is caused by the energy gap that occurs at graphene oxidation. Thermal conductivity of graphene also decreases as the number of the absorbed radicals increases. The absorbed radicals act as the scattering centers for phonons, hindering collisionless movement along the specimen. There are some processes that remove radicals by heat or chemical treatment. To sum up, reliable data on type and amount of adsorbed radicals are necessary in addition to geometry and object structure characteristics for unambiguous characterization of the object as well as for data evaluation. Hence, the measured properties of nanoobjects have unremovable uncertainty that stems from their atomic structure. Nevertheless, needs of engineering design or scientific research demand, that the property data have a certain certification of quality or an integrated estimation of uncertainty. This estimation should be based on accessible data on size and structure of object, method of measurement, method of synthesis, etc. Some more details are considered in section 6.|  | Figure 1. Schematic description of data system designing | 
|  | Figure 2. Schematic of the nanoscale objects characterization | 
|  | Figure 3. Data block “extra-factors” | 
|  | Figure 4. Schematic of the data certification | 
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| [1] | A.O. Erkimbaev, V.Yu. Zitserman, G.A. Kobzev, "Systematization of Data on the Physical and Chemical Properties and Application of Carbon Nanostructures", High Temperature, vol.48, no.6, pp.830–836, 2010. | 
| [2] | Y. Hu, O.A. Shenderova, D.W. Brenner, "Carbon Nanostructures: Morphologies and Properties", Journal of Computational and Theoretical Nanoscience, vol.4, no.2, pp.199-221, 2007. | 
| [3] | A.V. Eletskii, "Carbon nanotubes", Physics Uspehi, vol.40, no.9, 899–924, 1997. | 
| [4] | A.V. Eletskii, "Carbon nanotubes and their emission properties", Physics Uspehi, vol.45, no.4, pp.369–402, 2002. | 
| [5] | A.V. Eletskii, "Sorption properties of carbon nanostructures", Physics Uspehi, vol.47, no.11, pp.1119–1154, 2004. | 
| [6] | A.V. Eletskii, "Mechanical properties of carbon nanostructures and related materials", Physics Uspehi, vol.50, no.3, pp.225–261, 2007. | 
| [7] | A.V. Eletskii, "Transport properties of carbon nanotubes". Physics Uspehi, vol.52, no.3, pp.209–224, 2009. | 
| [8] | R.S. Berry, B.M. Smirnov, "Phase transitions in various kinds of clusters", Physics Uspehi, vol.52, no.9, pp.137–164, 2009. | 
| [9] | C.C. Yang, S. Li, "Size-Dependent Temperature−Pressure Phase Diagram of Carbon", J. Phys. Chem. C, vol.112, no.5, pp.1423-1426, 2008. | 
| [10] | E. Brown, L. Hao, J.C. Gallop, J.C. Macfarlane, "Ballistic thermal and electrical conductance measurements on individual multiwall carbon nanotubes", Appl. Phys. Lett., vol.87, Ar# 023107, 2005. | 
| [11] | А.V. Eletskii, I.M. Iskandarova, А.А. Knizhnik, D.N. Krasikov, "Graphene: fabrication methods and thermophysical properties", Physics Uspechi, vol.181, no.3, pp.233-268, 2011. | 
| [12] | S. Ghosh, W. Bao, D.L. Nika, S. Subrina, E.P. Pokatilov, C.N. Lau, A.A. Balandin, "Dimensional crossover of thermal transport in few-layer grapheme", Nature Materials, vol.9, no.7, pp.555-558, 2010. | 
| [13] | H.J. Li, W.G. Lu, J.J. Li, X.D. Bai, C.Z. Gu, "Multichannel Ballistic Transport in Multiwall Carbon Nanotubes", Phys. Rev. Lett., vol.95, Ar#086601, 2005. | 
| [14] | D.L. Nika, E.P. Pokatilov, A.S. Askerov, A.A. Balandin, "Phonon thermal conduction in grapheme: Role of Umklapp and edge roughness scattering", Phys. Rev. B, vol.79, Ar#155413, 2009. | 
| [15] | I.P. Suzdalev, P.I. Suzdalev, "Nanoclusters and nanocluster systems. Assembling, interactions and properties", Russian Chemical Reviews, vol.70, no.3, pp,177–210, 2001. | 
| [16] | Z.J. Han, K. Ostrikov, "Controlled electronic transport in single-walled carbon nanotube networks: Selecting electron hopping and chemical dopping mechanisms", Appl. Phys. Lett., vol.96, Ar#233115, 2010. | 
| [17] | A.S. Lobach, L.I. Buravov, N.G. Spizyna, A.V. Eletskii, A.P. Dementyev, K.I. Maslakov, "Temperture-dependent resistance of Single-Walled Carbon Nanotube Films", Khimiya Vys. Energiy, vol.45, no.4, pp.1–7, 2011. | 
| [18] | Y. Hernandez, V. Nicolosi, M. Lotya, et al, "High-yield production of grapheme by liquid-phase exfoliation of graphite", Nature Nanotechnology, vol.3, no.9, pp.563-568, 2008. | 
| [19] | R.G. Munro, "Data Evaluation, Theory and Practice for Materials Properties", Special Publication 960-11. Washington, DC: Materials Science and Engineering Laboratory, NIST, 2003. | 
| [20] | B. Moniz, "Nomenclature and current standards for identificaton of engineering materials". In: Newton, C.H. (Ed.) Manual on the Building of Materials Databases. ASTM Manual Series: MNL 19. Philadelphia: American Society for Testing and Materials, 1993. | 
| [21] | C.H. Newton, (Ed.) Manual on the Building of Materials Databases. ASTM Manual Series: MNL 19. Philadelphia: American Society for Testing and Materials, 1993. | 
| [22] | A.O. Erkimbaev, V.Yu. Zitserman, G.A. Kobzev, L.R. Fokin, "The logical structure of physicochemical data: Problems of numerical data standartization and exchange", Russian Journal of Physical Chemistry A, vol.82, no.1, pp.15-25, 2008. | 
| [23] | V.V. Pokropivny, V.V. Skorokhod, "New dimensionality classifications of nanostructures", Physica E., vol.40, no.7, pp.2521-2525, 2008). | 
| [24] | M. Yu, I. Chaudhuri, C. Leahy, S.Y. Wu, C.S. Jayanthi, "Energetics, relative stabilities, and size-dependent properties of nanosized carbon clusters of different families: Fullerenes, bucky-diamond, icosahedral, and bulk-truncated structures", J. Chem. Phys., vol.130, Ar#184708, 2009. | 
| [25] | G. Benedek, P. Milani, V.G., Ralchenko (Eds.), "Nanostructured carbon for advanced applications", NATO Science Series. II. Mathematics, Physics and Chemistry – Vol. 24. Berlin, Heidelberg, Dordrecht, New York: Springer, 2001. | 
| [26] | S. Abiteboul, P. Buneman, S. Suciu, "Data on the Web: From Relations to Semistructured Data and XML", Burlington, Massachusetts: Morgan Kaufman Publishers, 2000. | 
| [27] | V.V. Diky, G.J. Kabo, "Thermodynamic properties of C60 and C70 fullerenes", Russian Chemical Reviews, vol.69, no.2, pp.95-104, 2000. | 
| [28] | M. Graves, Designing XML Databases., Jersey: Prentice Hall, 2002. |