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dc.contributor.authorVega Lerín, Fidel
dc.contributor.authorPelaez de Fuentes, Ramon Javier
dc.contributor.authorKhun, Timo
dc.contributor.authorAfonso Rodriguez, Carmen Nieves
dc.contributor.authorRecio Sanchez, Gonzalo
dc.contributor.authorMartin Palma, Raul Jose
dc.contributor.otherUniversitat Politècnica de Catalunya. Departament d'Òptica i Optometria
dc.date.accessioned2014-11-04T12:42:54Z
dc.date.available2014-11-04T12:42:54Z
dc.date.created2014-05-14
dc.date.issued2014-05-14
dc.identifier.citationVega, F. [et al.]. Ultraviolet laser patterning of porous silicon. "Journal of applied physics", 14 Maig 2014, vol. 115, núm. 18, p. 184902-1-184902-8.
dc.identifier.issn0021-8979
dc.identifier.urihttp://hdl.handle.net/2117/24544
dc.description.abstractThis work reports on the fabrication of 1D fringed patterns on nanostructured porous silicon (nanoPS) layers (563, 372, and 290nm thick). The patterns are fabricated by phase-mask laser interference using single pulses of an UV excimer laser (193nm, 20ns pulse duration). The method is a single-step and flexible approach to produce a large variety of patterns formed by alternate regions of almost untransformed nanoPS and regions where its surface has melted and transformed into Si nanoparticles (NPs). The role of laser fluence (5-80mJcm-2), and pattern period (6.3-16µm) on pattern features and surface structuring are discussed. The results show that the diameter of Si NPs increases with fluence up to a saturation value of 75nm for a fluence ˜40mJcm-2. In addition, the percentage of transformed to non-transformed region normalized to the pattern period follows similar fluence dependence regardless the period and thus becomes an excellent control parameter. This dependence is fitted within a thermal model that allows for predicting the in-depth profile of the pattern. The model assumes that transformation occurs whenever the laser-induced temperature increase reaches the melting temperature of nanoPS that has been found to be 0.7 of that of crystalline silicon for a porosity of around 79%. The role of thermal gradients across the pattern is discussed in the light of the experimental results and the calculated temperature profiles, and shows that the contribution of lateral thermal flow to melting is not significant for pattern periods =6.3µm.
dc.language.isoeng
dc.publisherAmerican Institute of Physics (AIP)
dc.rightsAttribution-NonCommercial-NoDerivs 3.0 Spain
dc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/3.0/es/
dc.subjectÀrees temàtiques de la UPC::Enginyeria electrònica::Optoelectrònica::Làser
dc.subjectÀrees temàtiques de la UPC::Enginyeria dels materials
dc.subjectÀrees temàtiques de la UPC::Física
dc.subject.lcshUltraviolet radiation
dc.subject.lcshLasers
dc.subject.lcshPorous silicon
dc.subject.lcshNanosilicon
dc.subject.otherAcronym
dc.subject.otherSponsor: DAAD
dc.subject.otherGerman Academic Exchange Service
dc.titleUltraviolet laser patterning of porous silicon
dc.typeArticle
dc.subject.lemacLàsers
dc.subject.lemacRaigs ultraviolats
dc.subject.lemacMaterials nanoestructurals
dc.subject.lemacSilicones
dc.contributor.groupUniversitat Politècnica de Catalunya. GOAPI - Grup d'Òptica Aplicada i Processament d'Imatge
dc.identifier.doi10.1063/1.4875378
dc.relation.publisherversionhttp://scitation.aip.org/content/aip/journal/jap/115/18/10.1063/1.4875378
dc.rights.accessOpen Access
local.identifier.drac14938988
dc.description.versionPostprint (published version)
local.citation.authorVega, F.; Pelaez, R.; Khun, T.; Afonso, C.N.; Recio , G.; Martin, R.
local.citation.publicationNameJournal of applied physics
local.citation.volume115
local.citation.number18
local.citation.startingPage184902-1
local.citation.endingPage184902-8


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