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Influence of Bulk Temperature on Laser-Induced Periodic Surface Structures on Polycarbonate
In this paper, the influence of the bulk temperature (BT) of Polycarbonate (PC) on the occurrence and growth of Laser-induced Periodic Surface Structures (LIPSS) is studied. Ultrashort UV laser pulses with various laser peak fluence levels [Formula: see text] and various numbers of overscans [Formul...
Autores principales: | , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
MDPI
2019
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6960584/ https://www.ncbi.nlm.nih.gov/pubmed/31783566 http://dx.doi.org/10.3390/polym11121947 |
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author | Mezera, Marek Bonse, Jörn Römer, Gert-willem R. B. E. |
author_facet | Mezera, Marek Bonse, Jörn Römer, Gert-willem R. B. E. |
author_sort | Mezera, Marek |
collection | PubMed |
description | In this paper, the influence of the bulk temperature (BT) of Polycarbonate (PC) on the occurrence and growth of Laser-induced Periodic Surface Structures (LIPSS) is studied. Ultrashort UV laser pulses with various laser peak fluence levels [Formula: see text] and various numbers of overscans [Formula: see text] were applied on the surface of pre-heated Polycarbonate at different bulk temperatures. Increased BT leads to a stronger absorption of laser energy by the Polycarbonate. For [Formula: see text] High Spatial Frequency LIPSS (HSFL), Low Spatial Frequency LIPSS perpendicular (LSFL-I) and parallel (LSFL-II) to the laser polarization were only observed on the rim of the ablated tracks on the surface but not in the center of the tracks. For [Formula: see text] , it was found that when pre-heating the polymer to a BT close its glass transition temperature ([Formula: see text]), the laser fluence to achieve similar LIPSS as when processed at room temperature decreases by a factor of two. LSFL types I and II were obtained on PC at a BT close to [Formula: see text] and their periods and amplitudes were similar to typical values found in the literature. To the best of the author’s knowledge, it is the first time both LSFL types developed simultaneously and consistently on the same sample under equal laser processing parameters. The evolution of LIPSS from HSFL, over LSFL-II to LSFL I, is described, depending on laser peak fluence levels, number of pulses processing the spot and bulk temperature. |
format | Online Article Text |
id | pubmed-6960584 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2019 |
publisher | MDPI |
record_format | MEDLINE/PubMed |
spelling | pubmed-69605842020-01-23 Influence of Bulk Temperature on Laser-Induced Periodic Surface Structures on Polycarbonate Mezera, Marek Bonse, Jörn Römer, Gert-willem R. B. E. Polymers (Basel) Article In this paper, the influence of the bulk temperature (BT) of Polycarbonate (PC) on the occurrence and growth of Laser-induced Periodic Surface Structures (LIPSS) is studied. Ultrashort UV laser pulses with various laser peak fluence levels [Formula: see text] and various numbers of overscans [Formula: see text] were applied on the surface of pre-heated Polycarbonate at different bulk temperatures. Increased BT leads to a stronger absorption of laser energy by the Polycarbonate. For [Formula: see text] High Spatial Frequency LIPSS (HSFL), Low Spatial Frequency LIPSS perpendicular (LSFL-I) and parallel (LSFL-II) to the laser polarization were only observed on the rim of the ablated tracks on the surface but not in the center of the tracks. For [Formula: see text] , it was found that when pre-heating the polymer to a BT close its glass transition temperature ([Formula: see text]), the laser fluence to achieve similar LIPSS as when processed at room temperature decreases by a factor of two. LSFL types I and II were obtained on PC at a BT close to [Formula: see text] and their periods and amplitudes were similar to typical values found in the literature. To the best of the author’s knowledge, it is the first time both LSFL types developed simultaneously and consistently on the same sample under equal laser processing parameters. The evolution of LIPSS from HSFL, over LSFL-II to LSFL I, is described, depending on laser peak fluence levels, number of pulses processing the spot and bulk temperature. MDPI 2019-11-27 /pmc/articles/PMC6960584/ /pubmed/31783566 http://dx.doi.org/10.3390/polym11121947 Text en © 2019 by the authors. Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (http://creativecommons.org/licenses/by/4.0/). |
spellingShingle | Article Mezera, Marek Bonse, Jörn Römer, Gert-willem R. B. E. Influence of Bulk Temperature on Laser-Induced Periodic Surface Structures on Polycarbonate |
title | Influence of Bulk Temperature on Laser-Induced Periodic Surface Structures on Polycarbonate |
title_full | Influence of Bulk Temperature on Laser-Induced Periodic Surface Structures on Polycarbonate |
title_fullStr | Influence of Bulk Temperature on Laser-Induced Periodic Surface Structures on Polycarbonate |
title_full_unstemmed | Influence of Bulk Temperature on Laser-Induced Periodic Surface Structures on Polycarbonate |
title_short | Influence of Bulk Temperature on Laser-Induced Periodic Surface Structures on Polycarbonate |
title_sort | influence of bulk temperature on laser-induced periodic surface structures on polycarbonate |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6960584/ https://www.ncbi.nlm.nih.gov/pubmed/31783566 http://dx.doi.org/10.3390/polym11121947 |
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