Interior Melting of the C3B16 and C2B14− Clusters Between 1000 K and 2000 K

For bulk three-dimensional materials, it is common for the surface to melt at a slightly lower temperature than the bulk. This is known as surface melting, and is typically due to the fact that there are fewer bonds to surface atoms. However, for small clusters, this picture can change. In recent ye...

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Main Authors: Li-Ming Yang, Eric Ganz
Format: Article
Language:English
Published: MDPI AG 2017-11-01
Series:Condensed Matter
Subjects:
Online Access:https://www.mdpi.com/2410-3896/2/4/35
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spelling doaj-0fc1e55ce81e45bba637106c5ae993292020-11-24T20:48:26ZengMDPI AGCondensed Matter2410-38962017-11-01243510.3390/condmat2040035condmat2040035Interior Melting of the C3B16 and C2B14− Clusters Between 1000 K and 2000 KLi-Ming Yang0Eric Ganz1Key Laboratory of Material Chemistry for Energy Conversion and Storage, Ministry of Education, School of Chemistry and Chemical Engineering, Huazhong University of Science and Technology, Wuhan 430074, ChinaDepartment of Physics, University of Minnesota, 115 Union St., SE, Minneapolis, MN 55416, USAFor bulk three-dimensional materials, it is common for the surface to melt at a slightly lower temperature than the bulk. This is known as surface melting, and is typically due to the fact that there are fewer bonds to surface atoms. However, for small clusters, this picture can change. In recent years, there have been investigations of the B19 and B19− clusters, which show striking diffusive behavior as they are heated to 1000 K. We wondered what the effect of substituting a few carbon atoms would be on the properties of these small clusters. To this end, we carried out extensive structural searches and molecular dynamics simulations to study the properties of C3B16 and C2B14− at elevated temperatures. The ground state structures and lowest energy isomers for these clusters were determined and calculated. The lowest energy structures are two-dimensional with vacancies inside. The C atoms are located in the outer ring in the ground state. At 1400 K, the outer rim containing the carbon atoms has fixed bonding, while the interior atoms are able to diffuse freely. Therefore, both of these clusters display interior melting at 1400 K. This interior melting is explained by the larger bond strength of the rim atoms. Molecular dynamics simulations at 3000 K showed complete melting and we observed a wide variety of configurations in both clusters.https://www.mdpi.com/2410-3896/2/4/35boron clustersboron-carbon mixed clustersdensity functional theorymelting
collection DOAJ
language English
format Article
sources DOAJ
author Li-Ming Yang
Eric Ganz
spellingShingle Li-Ming Yang
Eric Ganz
Interior Melting of the C3B16 and C2B14− Clusters Between 1000 K and 2000 K
Condensed Matter
boron clusters
boron-carbon mixed clusters
density functional theory
melting
author_facet Li-Ming Yang
Eric Ganz
author_sort Li-Ming Yang
title Interior Melting of the C3B16 and C2B14− Clusters Between 1000 K and 2000 K
title_short Interior Melting of the C3B16 and C2B14− Clusters Between 1000 K and 2000 K
title_full Interior Melting of the C3B16 and C2B14− Clusters Between 1000 K and 2000 K
title_fullStr Interior Melting of the C3B16 and C2B14− Clusters Between 1000 K and 2000 K
title_full_unstemmed Interior Melting of the C3B16 and C2B14− Clusters Between 1000 K and 2000 K
title_sort interior melting of the c3b16 and c2b14− clusters between 1000 k and 2000 k
publisher MDPI AG
series Condensed Matter
issn 2410-3896
publishDate 2017-11-01
description For bulk three-dimensional materials, it is common for the surface to melt at a slightly lower temperature than the bulk. This is known as surface melting, and is typically due to the fact that there are fewer bonds to surface atoms. However, for small clusters, this picture can change. In recent years, there have been investigations of the B19 and B19− clusters, which show striking diffusive behavior as they are heated to 1000 K. We wondered what the effect of substituting a few carbon atoms would be on the properties of these small clusters. To this end, we carried out extensive structural searches and molecular dynamics simulations to study the properties of C3B16 and C2B14− at elevated temperatures. The ground state structures and lowest energy isomers for these clusters were determined and calculated. The lowest energy structures are two-dimensional with vacancies inside. The C atoms are located in the outer ring in the ground state. At 1400 K, the outer rim containing the carbon atoms has fixed bonding, while the interior atoms are able to diffuse freely. Therefore, both of these clusters display interior melting at 1400 K. This interior melting is explained by the larger bond strength of the rim atoms. Molecular dynamics simulations at 3000 K showed complete melting and we observed a wide variety of configurations in both clusters.
topic boron clusters
boron-carbon mixed clusters
density functional theory
melting
url https://www.mdpi.com/2410-3896/2/4/35
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