HCP track calculations in Lif:Mg,Ti: 3D modeling of the "track – escape" parameter
The conceptual framework of the track interaction model (TIM) was conceived in the 1970s and mathematically formulated in the 1980s to describe heavy charged particle TL fluence response supralinearity. The extended track interaction model (ETIM) was developed to include saturation effects due to ov...
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description | The conceptual framework of the track interaction model (TIM) was conceived in the 1970s and mathematically formulated in the 1980s to describe heavy charged particle TL fluence response supralinearity. The extended track interaction model (ETIM) was developed to include saturation effects due to overlapping tracks and has been applied to both proton and alpha particle TL fluence response. One of the parameters of major importance in the TIM is the "track – escape" parameter, defined by N
e/N
w, where N
e represents the number of electrons which escape the parent track during heating, and N
w is the number of electrons which recombine within the parent track to produce a TL photon. Recently a first attempt was carried out to theoretically model escape parameters calculated in 2D geometry as a function of particle type and energy using trapping center (TC), luminescent center (LC) and competitive center (CC) occupation probabilities calculated from track segment radial dose distributions and optical absorption (OA) dose response. In this study, the calculations are extended to 3D geometry using a Monte Carlo approach which samples the point of creation of the charge carriers according to the TC occupation probabilities and then estimates N
w by sampling the chord length to the track exterior. Charge carriers which escape the irradiated track volume contribute to N
e. This more sophisticated 3D calculation of N
e/N
w is expected to increase the reliability of the modeling of heavy charged particle TL fluence response in the framework of the ETIM and enhance our understanding of “track effects” in Heavy Charged Particle (HCP) induced TL. |
doi_str_mv | 10.1016/j.radmeas.2011.04.033 |
format | Article |
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e/N
w, where N
e represents the number of electrons which escape the parent track during heating, and N
w is the number of electrons which recombine within the parent track to produce a TL photon. Recently a first attempt was carried out to theoretically model escape parameters calculated in 2D geometry as a function of particle type and energy using trapping center (TC), luminescent center (LC) and competitive center (CC) occupation probabilities calculated from track segment radial dose distributions and optical absorption (OA) dose response. In this study, the calculations are extended to 3D geometry using a Monte Carlo approach which samples the point of creation of the charge carriers according to the TC occupation probabilities and then estimates N
w by sampling the chord length to the track exterior. Charge carriers which escape the irradiated track volume contribute to N
e. This more sophisticated 3D calculation of N
e/N
w is expected to increase the reliability of the modeling of heavy charged particle TL fluence response in the framework of the ETIM and enhance our understanding of “track effects” in Heavy Charged Particle (HCP) induced TL.</description><identifier>ISSN: 1350-4487</identifier><identifier>EISSN: 1879-0925</identifier><identifier>DOI: 10.1016/j.radmeas.2011.04.033</identifier><language>eng</language><publisher>Kidlington: Elsevier Ltd</publisher><subject>Charged particles ; Earth sciences ; Earth, ocean, space ; Escape parameter ; Exact sciences and technology ; Extender track interaction model ; Fluence ; Geochronology ; Hexagonal cells ; Isotope geochemistry. Geochronology ; LiF:Mg,Ti ; Mathematical models ; Monte Carlo methods ; Occupation ; Parents ; Supralinearity ; Three dimensional</subject><ispartof>Radiation measurements, 2011-12, Vol.46 (12), p.1353-1356</ispartof><rights>2011 Elsevier Ltd</rights><rights>2015 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c405t-2505f93314eb47b5adc01a4d0842e67a997543457fc29e4499328eca347699183</citedby><cites>FETCH-LOGICAL-c405t-2505f93314eb47b5adc01a4d0842e67a997543457fc29e4499328eca347699183</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://www.sciencedirect.com/science/article/pii/S1350448711001594$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>309,310,314,776,780,785,786,3537,23909,23910,25118,27901,27902,65306</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=25377060$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Sattinger, D.</creatorcontrib><creatorcontrib>Sharon, A.</creatorcontrib><creatorcontrib>Horowitz, Y.S.</creatorcontrib><title>HCP track calculations in Lif:Mg,Ti: 3D modeling of the "track – escape" parameter</title><title>Radiation measurements</title><description>The conceptual framework of the track interaction model (TIM) was conceived in the 1970s and mathematically formulated in the 1980s to describe heavy charged particle TL fluence response supralinearity. The extended track interaction model (ETIM) was developed to include saturation effects due to overlapping tracks and has been applied to both proton and alpha particle TL fluence response. One of the parameters of major importance in the TIM is the "track – escape" parameter, defined by N
e/N
w, where N
e represents the number of electrons which escape the parent track during heating, and N
w is the number of electrons which recombine within the parent track to produce a TL photon. Recently a first attempt was carried out to theoretically model escape parameters calculated in 2D geometry as a function of particle type and energy using trapping center (TC), luminescent center (LC) and competitive center (CC) occupation probabilities calculated from track segment radial dose distributions and optical absorption (OA) dose response. In this study, the calculations are extended to 3D geometry using a Monte Carlo approach which samples the point of creation of the charge carriers according to the TC occupation probabilities and then estimates N
w by sampling the chord length to the track exterior. Charge carriers which escape the irradiated track volume contribute to N
e. This more sophisticated 3D calculation of N
e/N
w is expected to increase the reliability of the modeling of heavy charged particle TL fluence response in the framework of the ETIM and enhance our understanding of “track effects” in Heavy Charged Particle (HCP) induced TL.</description><subject>Charged particles</subject><subject>Earth sciences</subject><subject>Earth, ocean, space</subject><subject>Escape parameter</subject><subject>Exact sciences and technology</subject><subject>Extender track interaction model</subject><subject>Fluence</subject><subject>Geochronology</subject><subject>Hexagonal cells</subject><subject>Isotope geochemistry. Geochronology</subject><subject>LiF:Mg,Ti</subject><subject>Mathematical models</subject><subject>Monte Carlo methods</subject><subject>Occupation</subject><subject>Parents</subject><subject>Supralinearity</subject><subject>Three dimensional</subject><issn>1350-4487</issn><issn>1879-0925</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2011</creationdate><recordtype>article</recordtype><recordid>eNqFkE1r3DAQhk1ooWnan1AQgUIOtTuyRpaVSwnbfMGW9rA9i4k8TrT1x1byFnrLf8g_7C-pl11yzWnm8LzzDk-WfZBQSJDV53URqemZUlGClAVgAUodZceyNjYHW-pX86405Ii1eZO9TWkNAGgrfZytbhY_xBTJ_xKeOr_taArjkEQYxDK059_uP63CuVBfRT823IXhXoytmB5YnO5D_x6fBCdPGz4VG4rU88TxXfa6pS7x-8M8yX5eXa4WN_ny-_Xt4mKZewQ95aUG3VqlJPIdmjtNjQdJ2ECNJVeGrDUaFWrT-tIyorWqrNmTQlNZK2t1kp3t727i-HvLaXJ9SJ67jgYet8lJg2ik1QgvoyChrgGrckb1HvVxTCly6zYx9BT_ztCOq9zaHYS7nXAH6Gbhc-7joYJmIV0bafAhPYdLrYyBavfKlz3Hs5o_gaNLPvDguQmR_eSaMbzQ9B_WGpXP</recordid><startdate>20111201</startdate><enddate>20111201</enddate><creator>Sattinger, D.</creator><creator>Sharon, A.</creator><creator>Horowitz, Y.S.</creator><general>Elsevier Ltd</general><general>Elsevier</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7QH</scope><scope>7UA</scope><scope>C1K</scope><scope>F1W</scope><scope>H97</scope><scope>L.G</scope><scope>7SR</scope><scope>7SU</scope><scope>7U5</scope><scope>8FD</scope><scope>FR3</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>20111201</creationdate><title>HCP track calculations in Lif:Mg,Ti: 3D modeling of the "track – escape" parameter</title><author>Sattinger, D. ; Sharon, A. ; Horowitz, Y.S.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c405t-2505f93314eb47b5adc01a4d0842e67a997543457fc29e4499328eca347699183</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2011</creationdate><topic>Charged particles</topic><topic>Earth sciences</topic><topic>Earth, ocean, space</topic><topic>Escape parameter</topic><topic>Exact sciences and technology</topic><topic>Extender track interaction model</topic><topic>Fluence</topic><topic>Geochronology</topic><topic>Hexagonal cells</topic><topic>Isotope geochemistry. Geochronology</topic><topic>LiF:Mg,Ti</topic><topic>Mathematical models</topic><topic>Monte Carlo methods</topic><topic>Occupation</topic><topic>Parents</topic><topic>Supralinearity</topic><topic>Three dimensional</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Sattinger, D.</creatorcontrib><creatorcontrib>Sharon, A.</creatorcontrib><creatorcontrib>Horowitz, Y.S.</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Aqualine</collection><collection>Water Resources Abstracts</collection><collection>Environmental Sciences and Pollution Management</collection><collection>ASFA: Aquatic Sciences and Fisheries Abstracts</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) 3: Aquatic Pollution & Environmental Quality</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) Professional</collection><collection>Engineered Materials Abstracts</collection><collection>Environmental Engineering Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Engineering Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Radiation measurements</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Sattinger, D.</au><au>Sharon, A.</au><au>Horowitz, Y.S.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>HCP track calculations in Lif:Mg,Ti: 3D modeling of the "track – escape" parameter</atitle><jtitle>Radiation measurements</jtitle><date>2011-12-01</date><risdate>2011</risdate><volume>46</volume><issue>12</issue><spage>1353</spage><epage>1356</epage><pages>1353-1356</pages><issn>1350-4487</issn><eissn>1879-0925</eissn><abstract>The conceptual framework of the track interaction model (TIM) was conceived in the 1970s and mathematically formulated in the 1980s to describe heavy charged particle TL fluence response supralinearity. The extended track interaction model (ETIM) was developed to include saturation effects due to overlapping tracks and has been applied to both proton and alpha particle TL fluence response. One of the parameters of major importance in the TIM is the "track – escape" parameter, defined by N
e/N
w, where N
e represents the number of electrons which escape the parent track during heating, and N
w is the number of electrons which recombine within the parent track to produce a TL photon. Recently a first attempt was carried out to theoretically model escape parameters calculated in 2D geometry as a function of particle type and energy using trapping center (TC), luminescent center (LC) and competitive center (CC) occupation probabilities calculated from track segment radial dose distributions and optical absorption (OA) dose response. In this study, the calculations are extended to 3D geometry using a Monte Carlo approach which samples the point of creation of the charge carriers according to the TC occupation probabilities and then estimates N
w by sampling the chord length to the track exterior. Charge carriers which escape the irradiated track volume contribute to N
e. This more sophisticated 3D calculation of N
e/N
w is expected to increase the reliability of the modeling of heavy charged particle TL fluence response in the framework of the ETIM and enhance our understanding of “track effects” in Heavy Charged Particle (HCP) induced TL.</abstract><cop>Kidlington</cop><pub>Elsevier Ltd</pub><doi>10.1016/j.radmeas.2011.04.033</doi><tpages>4</tpages></addata></record> |
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subjects | Charged particles Earth sciences Earth, ocean, space Escape parameter Exact sciences and technology Extender track interaction model Fluence Geochronology Hexagonal cells Isotope geochemistry. Geochronology LiF:Mg,Ti Mathematical models Monte Carlo methods Occupation Parents Supralinearity Three dimensional |
title | HCP track calculations in Lif:Mg,Ti: 3D modeling of the "track – escape" parameter |
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