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dc.contributor.authorValdivia J.A., Kiwi M., Bringa E.M., Rogan J.es_CL
dc.contributor.authorValencia, Felipe J. [Núcleo de Matemáticas, Física & Estadística, Facultad de Ciencias, Universidad Mayor, Chile]es_CL
dc.contributor.authorGonzález, Rafael I. [Centro de Genómica y Bioinformatica, Facultad de Ciencias, Universidad Mayor, Chile]es_CL
dc.date.accessioned2020-08-12T14:11:55Z
dc.date.accessioned2020-08-12T18:13:23Z
dc.date.available2020-08-12T14:11:55Z
dc.date.available2020-08-12T18:13:23Z
dc.date.issued2017es_CL
dc.identifier.citationValencia, F. J., González, R. I., Valdivia, J. A., Kiwi, M., Bringa, E. M., & Rogan, J. (2017). Inducing porosity on hollow nanoparticles by hypervelocity impacts. The Journal of Physical Chemistry C, 121(33), 17856-17861.es_CL
dc.identifier.issn1932-7447es_CL
dc.identifier.urihttps://pubs.acs.org/doi/pdf/10.1021/acs.jpcc.7b03126es_CL
dc.identifier.urihttps://doi.org/10.1021/acs.jpcc.7b03126es_CL
dc.identifier.urihttp://repositorio.umayor.cl/xmlui/handle/sibum/6894
dc.description.abstractThe large surface-to-volume ratio of hollow palladium nanoparticles (hNPs) offers room to improve their hydrogen storage capacity as well as their catalytic activity. However, a less explored possibility is to use, in addition, the internal cavity. Here we explore, through classical molecular dynamics, the possibility of boring channels across the hNP wall by collision with solid Pd nanoprojectiles at high velocities, as well as their resilience to maintain their spherical geometry. We choose a stable hNP with an inner diameter of 13 nm and an outer diameter of 15 nm. The projectiles are Pd NPs of 1.5, 2.4, and 3.0 nm, respectively. We consider collision speeds between 3 and 15 km/s, with an impact parameter between 0 to 7 nm. Four different regimes, as a function of kinetic energy and impact parameter of the projectile, are found. For low speeds, the projectile is not able to penetrate the target and only creates surface craters. For a narrow range of intermediate speeds, the projectile enters the target, but the hNP shell is able to self-heal, either totally or partially. For large speeds, the projectile penetrates the target without altering its spherical hollow geometry, but for even larger speeds, the hNP collapses into a solid structure. The specific threshold speed for each regime depends on the mass and speed of the projectile. In all noncollapsing cases, the results show a linear relationship between projectile kinetic energy and crater or perforation size. We also studied its behavior when the hNP suffers successive collisions, finding that it keeps its hollow shape but forms faceted structures, such as nanoframes or hollow cuboctahedron nanoparticles. All of our results suggest that Pd hNPs, with adequate combinations of external radius and thickness are very robust, can withstand hypervelocity impacts and that channels can be opened to allow molecules to reach the internal cavity.es_CL
dc.description.sponsorshipThis work was supported by the Fondo Nacional de Investigaciones Cientificas y Tecnologicas (FONDECYT, Chile) under Grants #1160639 and 1130272 (M.K. and J.R.), 1150718 (J.A.V.) AFOSR Grant FA9550-16-1-0122 (J.A.V. and M.K.), and Financiamiento Basal para Centros Cientificos y Tecnologicos de Excelencia FB-0807 (RG., F.V., J.M., M.K., and J.R). E.M.B. thanks support from the PICT-2014-0696 (ANPCyT) and M003 (SeCTyP-UN Cuyo) Grants. F.V. was supported by CONICYT Doctoral Fellowship Grant 21140948.es_CL
dc.format.extentArtículo original
dc.language.isoenes_CL
dc.publisherAmerican Chemical Societyes_CL
dc.rightsAttribution-NonCommercial-NoDerivs 3.0 Chile
dc.sourceJournal of Physical Chemistry C, 2017. 121(33): p: 17856-17861
dc.titleInducing Porosity on Hollow Nanoparticles by Hypervelocity Impactses_CL
dc.typeArtículo o paperes_CL
umayor.facultadFacultad de Ciencias
umayor.indizadorCOT
umayor.politicas.sherpa/romeoRoMEO WHITE journal (El archivo no está formalmente admitido). Disponible en: http://sherpa.ac.uk/romeo/index.phpes_CL
umayor.indexadoWOSes_CL
umayor.indexadoSCOPUSes_CL
dc.identifier.doiDOI: 10.1021/acs.jpcc.7b03126es_CL]
umayor.indicadores.wos-(cuartil)Q2es_CL
umayor.indicadores.scopus-(scimago-sjr)1,48es_CL
umayor.indicadores.scopus-(scimago-sjr)ÍNDICE H: 6es_CL


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