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 F 0 and various numbers of overscans ( N OS ) were applied o...
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Veröffentlicht in: | Polymers 2019-11, Vol.11 (12), p.1947 |
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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 F 0 and various numbers of overscans ( N OS ) 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 N OS < 1000 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 N OS ≥ 1000 , it was found that when pre-heating the polymer to a BT close its glass transition temperature ( T g ), 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 T g 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. |
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Ultrashort UV laser pulses with various laser peak fluence levels F 0 and various numbers of overscans ( N OS ) 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 N OS < 1000 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 N OS ≥ 1000 , it was found that when pre-heating the polymer to a BT close its glass transition temperature ( T g ), 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 T g 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.</description><identifier>ISSN: 2073-4360</identifier><identifier>EISSN: 2073-4360</identifier><identifier>DOI: 10.3390/polym11121947</identifier><identifier>PMID: 31783566</identifier><language>eng</language><publisher>Switzerland: MDPI AG</publisher><subject>Ablation ; Fluence ; Glass transition temperature ; Laser processing ; Lasers ; Oxidation ; Polycarbonate resins ; Polymers ; Process parameters ; Radiation ; Room temperature ; Ultraviolet lasers</subject><ispartof>Polymers, 2019-11, Vol.11 (12), p.1947</ispartof><rights>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/). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><rights>2019 by the authors. 2019</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c415t-c574f8130cab3f8678e706ba94fafdd25a44a198cbf340eb91ff3dfeed9d49313</citedby><cites>FETCH-LOGICAL-c415t-c574f8130cab3f8678e706ba94fafdd25a44a198cbf340eb91ff3dfeed9d49313</cites><orcidid>0000-0003-4984-3896</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://www.ncbi.nlm.nih.gov/pmc/articles/PMC6960584/pdf/$$EPDF$$P50$$Gpubmedcentral$$Hfree_for_read</linktopdf><linktohtml>$$Uhttps://www.ncbi.nlm.nih.gov/pmc/articles/PMC6960584/$$EHTML$$P50$$Gpubmedcentral$$Hfree_for_read</linktohtml><link.rule.ids>230,314,727,780,784,885,27922,27923,53789,53791</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/31783566$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Mezera, Marek</creatorcontrib><creatorcontrib>Bonse, Jörn</creatorcontrib><creatorcontrib>Römer, Gert-Willem R B E</creatorcontrib><title>Influence of Bulk Temperature on Laser-Induced Periodic Surface Structures on Polycarbonate</title><title>Polymers</title><addtitle>Polymers (Basel)</addtitle><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 F 0 and various numbers of overscans ( N OS ) 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 N OS < 1000 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 N OS ≥ 1000 , it was found that when pre-heating the polymer to a BT close its glass transition temperature ( T g ), 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 T g 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.</description><subject>Ablation</subject><subject>Fluence</subject><subject>Glass transition temperature</subject><subject>Laser processing</subject><subject>Lasers</subject><subject>Oxidation</subject><subject>Polycarbonate resins</subject><subject>Polymers</subject><subject>Process parameters</subject><subject>Radiation</subject><subject>Room temperature</subject><subject>Ultraviolet lasers</subject><issn>2073-4360</issn><issn>2073-4360</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><recordid>eNpdkc1LNSEUxiWKilvLtjHwbtpM6agz4yZ4iz4uXCioVi3E0WNNzehNx6D_Pi99ULlRjz-f8xwehPYIPqRU4KOlH95GQkhFBGvW0HaFG1oyWuP1H-cttBvjE86L8bomzSbaoqRpab5so_u5s0MCp6HwtjhJw3NxC-MSgppSyDVXLFSEUM6dSRpMcQ2h96bXxU0KVuVfN1NIesXGFXydDWkVOu_UBDtow6ohwu7nPkN352e3p5fl4upifvp_UWpG-FRq3jDbEoq16qht66aFBtedEswqa0zFFWOKiFZ3ljIMnSDWUmMBjDBMUEJn6PhDd5m6EYwGNwU1yGXoRxXepFe9_P3i-kf54F9lLWrMW5YFDj4Fgn9JECc59lHDMCgHPkVZ0QrTRvB21evfH_TJp-DyeLLiHFe8qrOnGSo_KB18jAHstxmC5So5-Su5zO__nOCb_sqJvgND_Zaq</recordid><startdate>20191127</startdate><enddate>20191127</enddate><creator>Mezera, Marek</creator><creator>Bonse, Jörn</creator><creator>Römer, Gert-Willem R B E</creator><general>MDPI AG</general><general>MDPI</general><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SR</scope><scope>8FD</scope><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>D1I</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>JG9</scope><scope>KB.</scope><scope>PDBOC</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>7X8</scope><scope>5PM</scope><orcidid>https://orcid.org/0000-0003-4984-3896</orcidid></search><sort><creationdate>20191127</creationdate><title>Influence of Bulk Temperature on Laser-Induced Periodic Surface Structures on Polycarbonate</title><author>Mezera, Marek ; Bonse, Jörn ; Römer, Gert-Willem R B E</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c415t-c574f8130cab3f8678e706ba94fafdd25a44a198cbf340eb91ff3dfeed9d49313</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2019</creationdate><topic>Ablation</topic><topic>Fluence</topic><topic>Glass transition temperature</topic><topic>Laser processing</topic><topic>Lasers</topic><topic>Oxidation</topic><topic>Polycarbonate resins</topic><topic>Polymers</topic><topic>Process parameters</topic><topic>Radiation</topic><topic>Room temperature</topic><topic>Ultraviolet lasers</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Mezera, Marek</creatorcontrib><creatorcontrib>Bonse, Jörn</creatorcontrib><creatorcontrib>Römer, Gert-Willem R B E</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>Engineered Materials Abstracts</collection><collection>Technology Research Database</collection><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest Central UK/Ireland</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Materials Science Collection</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection</collection><collection>Materials Research Database</collection><collection>Materials Science Database</collection><collection>Materials Science Collection</collection><collection>Publicly Available Content Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><collection>MEDLINE - Academic</collection><collection>PubMed Central (Full Participant titles)</collection><jtitle>Polymers</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Mezera, Marek</au><au>Bonse, Jörn</au><au>Römer, Gert-Willem R B E</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Influence of Bulk Temperature on Laser-Induced Periodic Surface Structures on Polycarbonate</atitle><jtitle>Polymers</jtitle><addtitle>Polymers (Basel)</addtitle><date>2019-11-27</date><risdate>2019</risdate><volume>11</volume><issue>12</issue><spage>1947</spage><pages>1947-</pages><issn>2073-4360</issn><eissn>2073-4360</eissn><abstract>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 F 0 and various numbers of overscans ( N OS ) 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 N OS < 1000 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 N OS ≥ 1000 , it was found that when pre-heating the polymer to a BT close its glass transition temperature ( T g ), 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 T g 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.</abstract><cop>Switzerland</cop><pub>MDPI AG</pub><pmid>31783566</pmid><doi>10.3390/polym11121947</doi><orcidid>https://orcid.org/0000-0003-4984-3896</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | Ablation Fluence Glass transition temperature Laser processing Lasers Oxidation Polycarbonate resins Polymers Process parameters Radiation Room temperature Ultraviolet lasers |
title | Influence of Bulk Temperature on Laser-Induced Periodic Surface Structures on Polycarbonate |
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