Please use this identifier to cite or link to this item: https://hdl.handle.net/20.500.14279/1379
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dc.contributor.authorKelires, Pantelis C.-
dc.date.accessioned2013-03-06T16:33:41Zen
dc.date.accessioned2013-05-17T05:22:59Z-
dc.date.accessioned2015-12-02T10:18:08Z-
dc.date.available2013-03-06T16:33:41Zen
dc.date.available2013-05-17T05:22:59Z-
dc.date.available2015-12-02T10:18:08Z-
dc.date.issued1993-
dc.identifier.citationPhysical Review B,1993, vol. 47, no. 4, pp. 1829-1839en_US
dc.identifier.issn01631829-
dc.identifier.urihttps://hdl.handle.net/20.500.14279/1379-
dc.description.abstractWe have made a comparative theoretical study of the most common forms of unhydrogenated amorphous carbon (α-C), namely, of the dense, diamondlike phase and the low-density evaporated α-C (e-C). Emphasis is given to the connection among the structure, energetics, and stability of these phases. To make the simulations of the amorphous structures (formed by quenching the liquid) tractable, we used the Monte Carlo method, combined with the empirical-potential approach. Our analysis employs a powerful total-energy-partitioning scheme, which is proved very useful in treating the energetics of disordered systems. It is found that threefold sp2 sites are the energetically favorable geometries in e-C, and thus they are by far more numerous. The nonplanar character of sp2 sites and the absence of sixfold rings indicate that medium-range order is rather not significant in e-C. The increasing graphitic character of e-C, as the temperature is raised, is explained by resorting to the effective temperatures T*, at which the atoms freeze in their lattice positions. For diamondlike α-C, the simulations show that there exist two distinctly different dense structures. The ''as-quenched'' one (i-C) is mostly sp3 bonded, but it is metastable. Upon annealing, it converts into a second phase (i-C*), mostly sp2 bonded, with a significant energy gain. A specific mechanism is proposed for this transition. The insensitivity of density to annealing is explained if we use the concept of the ''glass transition temperature'' T*. Finally, by introducing an isotropic bulk modulus for the amorphous phase, it is found that e-C has a much lower compressibility than i-C*, enhancing the distinguishability among the two low-coordinated forms of α-C.en_US
dc.formatpdfen_US
dc.language.isoenen_US
dc.relation.ispartofPhysical Review Ben_US
dc.rights© American Physical Societyen_US
dc.subjectCarbonen_US
dc.subjectMonte Carlo methoden_US
dc.subjectDensityen_US
dc.titleStructural properties and energetics of amorphous forms of carbonen_US
dc.typeArticleen_US
dc.collaborationUniversity of Creteen_US
dc.collaborationResearch Center of Creteen_US
dc.subject.categoryMechanical Engineeringen_US
dc.journalsHybrid Open Accessen_US
dc.countryGreeceen_US
dc.subject.fieldEngineering and Technologyen_US
dc.publicationPeer Revieweden_US
dc.identifier.doi10.1103/PhysRevB.47.1829en_US
dc.dept.handle123456789/54en
dc.relation.issue4en_US
dc.relation.volume47en_US
cut.common.academicyear2020-2021en_US
dc.identifier.spage1829en_US
dc.identifier.epage1839en_US
item.languageiso639-1en-
item.cerifentitytypePublications-
item.fulltextNo Fulltext-
item.grantfulltextnone-
item.openairetypearticle-
item.openairecristypehttp://purl.org/coar/resource_type/c_6501-
crisitem.author.deptDepartment of Mechanical Engineering and Materials Science and Engineering-
crisitem.author.facultyFaculty of Engineering and Technology-
crisitem.author.orcid0000-0002-0268-259X-
crisitem.author.parentorgFaculty of Engineering and Technology-
crisitem.journal.journalissn2469-9969-
crisitem.journal.publisherAmerican Physical Society-
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