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Role of wavelength in photocarrier absorption and plasma formation threshold under excitation of dielectrics by high-intensity laser field tunable from visible to mid-IR
The development of high power mid-IR laser applications requires a study on laser induced damage threshold (LIDT) in the mid-IR. In this paper we have measured the wavelength dependence of the plasma formation threshold (PFT) that is a LIDT precursor. In order to interpret the observed trends numeri...
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Published in: | Scientific reports 2020-08, Vol.10 (1), p.14007-14007, Article 14007 |
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description | The development of high power mid-IR laser applications requires a study on laser induced damage threshold (LIDT) in the mid-IR. In this paper we have measured the wavelength dependence of the plasma formation threshold (PFT) that is a LIDT precursor. In order to interpret the observed trends numerically, a model describing the laser induced electron dynamics, based on multiple rate equations, has been developed. We show both theoretically and experimentally that PFT at mid-IR wavelengths is controlled by a transition from weak- to strong-field regime of free carrier absorption. In the case of MgF
2
this transition occurs around 3–4
μ
m corresponding to the region of the lowermost PFT. The region of the uppermost PFT is reached around 1
μ
m and is governed by an interplay of photoionization and weak-field free carrier absorption which manifests itself in both MgF
2
and SiO
2
. The PFT observed in considered materials exhibits a universal dependence on the excitation wavelength in dielectrics. Thus, the presented results pave the route towards efficient and controllable laser-induced material modifications and should be of direct interest to laser researchers and application engineers for prevention of laser-induced damage of optical components in high-intensity mid-IR laser systems. |
doi_str_mv | 10.1038/s41598-020-70862-w |
format | article |
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2
this transition occurs around 3–4
μ
m corresponding to the region of the lowermost PFT. The region of the uppermost PFT is reached around 1
μ
m and is governed by an interplay of photoionization and weak-field free carrier absorption which manifests itself in both MgF
2
and SiO
2
. The PFT observed in considered materials exhibits a universal dependence on the excitation wavelength in dielectrics. Thus, the presented results pave the route towards efficient and controllable laser-induced material modifications and should be of direct interest to laser researchers and application engineers for prevention of laser-induced damage of optical components in high-intensity mid-IR laser systems.</description><identifier>ISSN: 2045-2322</identifier><identifier>EISSN: 2045-2322</identifier><identifier>DOI: 10.1038/s41598-020-70862-w</identifier><identifier>PMID: 32814797</identifier><language>eng</language><publisher>London: Nature Publishing Group UK</publisher><subject>639/301/119/995 ; 639/624/400/385 ; 639/624/400/584 ; 639/766/1960/1135 ; Absorption ; Humanities and Social Sciences ; Lasers ; multidisciplinary ; Science ; Science (multidisciplinary) ; Silicon dioxide ; Wavelength ; Wavelengths</subject><ispartof>Scientific reports, 2020-08, Vol.10 (1), p.14007-14007, Article 14007</ispartof><rights>The Author(s) 2020</rights><rights>The Author(s) 2020. This work is published under http://creativecommons.org/licenses/by/4.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c474t-717abdf4acbc9d1b56b3c19d9d2d2a7e6fcfe288a304c853c577785e3c20792e3</citedby><cites>FETCH-LOGICAL-c474t-717abdf4acbc9d1b56b3c19d9d2d2a7e6fcfe288a304c853c577785e3c20792e3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://www.proquest.com/docview/2435332661/fulltextPDF?pq-origsite=primo$$EPDF$$P50$$Gproquest$$Hfree_for_read</linktopdf><linktohtml>$$Uhttps://www.proquest.com/docview/2435332661?pq-origsite=primo$$EHTML$$P50$$Gproquest$$Hfree_for_read</linktohtml><link.rule.ids>230,314,727,780,784,885,25753,27924,27925,37012,37013,44590,53791,53793,75126</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/32814797$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Migal, Ekaterina</creatorcontrib><creatorcontrib>Mareev, Evgenii</creatorcontrib><creatorcontrib>Smetanina, Evgeniya</creatorcontrib><creatorcontrib>Duchateau, Guillaume</creatorcontrib><creatorcontrib>Potemkin, Fedor</creatorcontrib><title>Role of wavelength in photocarrier absorption and plasma formation threshold under excitation of dielectrics by high-intensity laser field tunable from visible to mid-IR</title><title>Scientific reports</title><addtitle>Sci Rep</addtitle><addtitle>Sci Rep</addtitle><description>The development of high power mid-IR laser applications requires a study on laser induced damage threshold (LIDT) in the mid-IR. In this paper we have measured the wavelength dependence of the plasma formation threshold (PFT) that is a LIDT precursor. In order to interpret the observed trends numerically, a model describing the laser induced electron dynamics, based on multiple rate equations, has been developed. We show both theoretically and experimentally that PFT at mid-IR wavelengths is controlled by a transition from weak- to strong-field regime of free carrier absorption. In the case of MgF
2
this transition occurs around 3–4
μ
m corresponding to the region of the lowermost PFT. The region of the uppermost PFT is reached around 1
μ
m and is governed by an interplay of photoionization and weak-field free carrier absorption which manifests itself in both MgF
2
and SiO
2
. The PFT observed in considered materials exhibits a universal dependence on the excitation wavelength in dielectrics. 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Mareev, Evgenii ; Smetanina, Evgeniya ; Duchateau, Guillaume ; Potemkin, Fedor</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c474t-717abdf4acbc9d1b56b3c19d9d2d2a7e6fcfe288a304c853c577785e3c20792e3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2020</creationdate><topic>639/301/119/995</topic><topic>639/624/400/385</topic><topic>639/624/400/584</topic><topic>639/766/1960/1135</topic><topic>Absorption</topic><topic>Humanities and Social Sciences</topic><topic>Lasers</topic><topic>multidisciplinary</topic><topic>Science</topic><topic>Science (multidisciplinary)</topic><topic>Silicon dioxide</topic><topic>Wavelength</topic><topic>Wavelengths</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Migal, Ekaterina</creatorcontrib><creatorcontrib>Mareev, Evgenii</creatorcontrib><creatorcontrib>Smetanina, Evgeniya</creatorcontrib><creatorcontrib>Duchateau, Guillaume</creatorcontrib><creatorcontrib>Potemkin, Fedor</creatorcontrib><collection>SpringerOpen</collection><collection>PubMed</collection><collection>CrossRef</collection><collection>ProQuest Central (Corporate)</collection><collection>Health & Medical Collection</collection><collection>ProQuest Central (purchase pre-March 2016)</collection><collection>Biology Database (Alumni Edition)</collection><collection>Medical Database (Alumni Edition)</collection><collection>Science Database (Alumni Edition)</collection><collection>ProQuest SciTech Collection</collection><collection>ProQuest Natural Science Collection</collection><collection>Hospital Premium Collection</collection><collection>Hospital Premium Collection (Alumni Edition)</collection><collection>ProQuest Central (Alumni) (purchase pre-March 2016)</collection><collection>ProQuest Central (Alumni)</collection><collection>ProQuest Central</collection><collection>ProQuest Central Essentials</collection><collection>Biological Science Collection</collection><collection>ProQuest Central</collection><collection>Natural Science Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central</collection><collection>Health Research Premium Collection</collection><collection>Health Research Premium Collection (Alumni)</collection><collection>ProQuest Central Student</collection><collection>SciTech Premium Collection</collection><collection>ProQuest Health & Medical Complete (Alumni)</collection><collection>ProQuest Biological Science Collection</collection><collection>Health & Medical Collection (Alumni Edition)</collection><collection>PML(ProQuest Medical Library)</collection><collection>Science Database (ProQuest)</collection><collection>Biological Science Database</collection><collection>Publicly Available Content (ProQuest)</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 Basic</collection><collection>MEDLINE - Academic</collection><collection>PubMed Central (Full Participant titles)</collection><jtitle>Scientific reports</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Migal, Ekaterina</au><au>Mareev, Evgenii</au><au>Smetanina, Evgeniya</au><au>Duchateau, Guillaume</au><au>Potemkin, Fedor</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Role of wavelength in photocarrier absorption and plasma formation threshold under excitation of dielectrics by high-intensity laser field tunable from visible to mid-IR</atitle><jtitle>Scientific reports</jtitle><stitle>Sci Rep</stitle><addtitle>Sci Rep</addtitle><date>2020-08-19</date><risdate>2020</risdate><volume>10</volume><issue>1</issue><spage>14007</spage><epage>14007</epage><pages>14007-14007</pages><artnum>14007</artnum><issn>2045-2322</issn><eissn>2045-2322</eissn><abstract>The development of high power mid-IR laser applications requires a study on laser induced damage threshold (LIDT) in the mid-IR. In this paper we have measured the wavelength dependence of the plasma formation threshold (PFT) that is a LIDT precursor. In order to interpret the observed trends numerically, a model describing the laser induced electron dynamics, based on multiple rate equations, has been developed. We show both theoretically and experimentally that PFT at mid-IR wavelengths is controlled by a transition from weak- to strong-field regime of free carrier absorption. In the case of MgF
2
this transition occurs around 3–4
μ
m corresponding to the region of the lowermost PFT. The region of the uppermost PFT is reached around 1
μ
m and is governed by an interplay of photoionization and weak-field free carrier absorption which manifests itself in both MgF
2
and SiO
2
. The PFT observed in considered materials exhibits a universal dependence on the excitation wavelength in dielectrics. Thus, the presented results pave the route towards efficient and controllable laser-induced material modifications and should be of direct interest to laser researchers and application engineers for prevention of laser-induced damage of optical components in high-intensity mid-IR laser systems.</abstract><cop>London</cop><pub>Nature Publishing Group UK</pub><pmid>32814797</pmid><doi>10.1038/s41598-020-70862-w</doi><tpages>1</tpages><oa>free_for_read</oa></addata></record> |
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subjects | 639/301/119/995 639/624/400/385 639/624/400/584 639/766/1960/1135 Absorption Humanities and Social Sciences Lasers multidisciplinary Science Science (multidisciplinary) Silicon dioxide Wavelength Wavelengths |
title | Role of wavelength in photocarrier absorption and plasma formation threshold under excitation of dielectrics by high-intensity laser field tunable from visible to mid-IR |
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