FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2016506089> ?p ?o ?g. }

• W2016506089 abstract "The ability of the classical nucleation theory (CNT) and atomistic nucleation theory (ANT) to predict the stationary nucleation rate J of single-component crystals and crystalline monolayers is verified with the aid of numerical and computer simulation data obtained in the scope of the Kossel crystal model. It is found that in both cases CNT significantly overestimates J because it does not account for the work needed to attach an atom to the periphery of the two-dimensional nucleus or to form such a nucleus on the surface of the three-dimensional one. In contrast, ANT is successful in providing a good quantitative description of J, especially for high enough effective binding energy between nearest-neighbor atoms in the crystal and in capturing the existence of extended, nearly linear portions in the dependence of ln J on the supersaturation s when the values of both s and the binding energy are sufficiently great. However, the ANT prediction about broken linear ln J versus s dependence is not confirmed by the numerical and simulation results presented. General formulas for the nucleation work, the nucleus size, and the nucleation rate are proposed which are applicable to nucleation of single-component crystals and crystalline monolayers in vapors, solutions, or melts and which correct the respective CNT formulas. The proposed J(s) formula provides a good description of the numerical and simulation data and can justifiably be used up to the supersaturation at which the nucleus becomes monomer. When experimental data for the J(s) dependence are available and the nucleus specific edge and surface energies are unknown parameters, the proposed J(s) formula can be employed for estimation of these energies even if the nucleus is constituted of a few atoms only." @default.
• W2016506089 created "2016-06-24" @default.
• W2016506089 creator A5073436350 @default.
• W2016506089 date "2008-10-22" @default.
• W2016506089 modified "2023-10-16" @default.
• W2016506089 title "Toward a better description of the nucleation rate of crystals and crystalline monolayers" @default.
• W2016506089 cites W151306072 @default.
• W2016506089 cites W1568812877 @default.
• W2016506089 cites W159425321 @default.
• W2016506089 cites W1644550153 @default.
• W2016506089 cites W1964414565 @default.
• W2016506089 cites W1965965771 @default.
• W2016506089 cites W1966175845 @default.
• W2016506089 cites W1969912598 @default.
• W2016506089 cites W1983834311 @default.
• W2016506089 cites W1987368754 @default.
• W2016506089 cites W1987444197 @default.
• W2016506089 cites W1997245777 @default.
• W2016506089 cites W2003089050 @default.
• W2016506089 cites W2003344028 @default.
• W2016506089 cites W2007105255 @default.
• W2016506089 cites W2013736497 @default.
• W2016506089 cites W2021868227 @default.
• W2016506089 cites W2025245808 @default.
• W2016506089 cites W2034641484 @default.
• W2016506089 cites W2035717876 @default.
• W2016506089 cites W2038667467 @default.
• W2016506089 cites W2039273770 @default.
• W2016506089 cites W2041635134 @default.
• W2016506089 cites W2043727418 @default.
• W2016506089 cites W2045405054 @default.
• W2016506089 cites W2057064580 @default.
• W2016506089 cites W2058802654 @default.
• W2016506089 cites W2061150119 @default.
• W2016506089 cites W2062308989 @default.
• W2016506089 cites W2062568637 @default.
• W2016506089 cites W2073717789 @default.
• W2016506089 cites W2078724502 @default.
• W2016506089 cites W2080797229 @default.
• W2016506089 cites W2081721619 @default.
• W2016506089 cites W2088197868 @default.
• W2016506089 cites W2095567101 @default.
• W2016506089 cites W2129641858 @default.
• W2016506089 cites W2135836384 @default.
• W2016506089 cites W4252653731 @default.
• W2016506089 cites W2003813593 @default.
• W2016506089 cites W2084123526 @default.
• W2016506089 doi "https://doi.org/10.1063/1.2996505" @default.
• W2016506089 hasPubMedId "https://pubmed.ncbi.nlm.nih.gov/19045292" @default.
• W2016506089 hasPublicationYear "2008" @default.
• W2016506089 type Work @default.
• W2016506089 sameAs 2016506089 @default.
• W2016506089 citedByCount "33" @default.
• W2016506089 countsByYear W20165060892012 @default.
• W2016506089 countsByYear W20165060892014 @default.
• W2016506089 countsByYear W20165060892015 @default.
• W2016506089 countsByYear W20165060892016 @default.
• W2016506089 countsByYear W20165060892017 @default.
• W2016506089 countsByYear W20165060892019 @default.
• W2016506089 countsByYear W20165060892021 @default.
• W2016506089 countsByYear W20165060892022 @default.
• W2016506089 countsByYear W20165060892023 @default.
• W2016506089 crossrefType "journal-article" @default.
• W2016506089 hasAuthorship W2016506089A5073436350 @default.
• W2016506089 hasConcept C121332964 @default.
• W2016506089 hasConcept C121864883 @default.
• W2016506089 hasConcept C149635348 @default.
• W2016506089 hasConcept C159467904 @default.
• W2016506089 hasConcept C171250308 @default.
• W2016506089 hasConcept C185592680 @default.
• W2016506089 hasConcept C18762648 @default.
• W2016506089 hasConcept C192562407 @default.
• W2016506089 hasConcept C195839 @default.
• W2016506089 hasConcept C199360897 @default.
• W2016506089 hasConcept C200447597 @default.
• W2016506089 hasConcept C2780393986 @default.
• W2016506089 hasConcept C2781285689 @default.
• W2016506089 hasConcept C41008148 @default.
• W2016506089 hasConcept C58312451 @default.
• W2016506089 hasConcept C61048295 @default.
• W2016506089 hasConcept C7070889 @default.
• W2016506089 hasConcept C8010536 @default.
• W2016506089 hasConcept C97355855 @default.
• W2016506089 hasConceptScore W2016506089C121332964 @default.
• W2016506089 hasConceptScore W2016506089C121864883 @default.
• W2016506089 hasConceptScore W2016506089C149635348 @default.
• W2016506089 hasConceptScore W2016506089C159467904 @default.
• W2016506089 hasConceptScore W2016506089C171250308 @default.
• W2016506089 hasConceptScore W2016506089C185592680 @default.
• W2016506089 hasConceptScore W2016506089C18762648 @default.
• W2016506089 hasConceptScore W2016506089C192562407 @default.
• W2016506089 hasConceptScore W2016506089C195839 @default.
• W2016506089 hasConceptScore W2016506089C199360897 @default.
• W2016506089 hasConceptScore W2016506089C200447597 @default.
• W2016506089 hasConceptScore W2016506089C2780393986 @default.
• W2016506089 hasConceptScore W2016506089C2781285689 @default.
• W2016506089 hasConceptScore W2016506089C41008148 @default.
• W2016506089 hasConceptScore W2016506089C58312451 @default.
• W2016506089 hasConceptScore W2016506089C61048295 @default.
• W2016506089 hasConceptScore W2016506089C7070889 @default.

• next