Experimental determination of the PTW 60019 microDiamond dosimeter active area and volume

Purpose: Small field output correction factors have been studied by several research groups for the PTW 60019 microDiamond (MD) dosimeter, by comparing the response of such a device with both reference dosimeters and Monte Carlo simulations. A general good agreement is observed for field sizes down...

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Veröffentlicht in:Medical physics (Lancaster) 2016-09, Vol.43 (9), p.5205-5212
Hauptverfasser: Marinelli, Marco, Prestopino, G., Verona, C., Verona-Rinati, G.
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container_issue 9
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creator Marinelli, Marco
Prestopino, G.
Verona, C.
Verona-Rinati, G.
description Purpose: Small field output correction factors have been studied by several research groups for the PTW 60019 microDiamond (MD) dosimeter, by comparing the response of such a device with both reference dosimeters and Monte Carlo simulations. A general good agreement is observed for field sizes down to about 1 cm. However, evident inconsistencies can be noticed when comparing some experimental results and Monte Carlo simulations obtained for smaller irradiation fields. This issue was tentatively attributed by some authors to unintentional large variations of the MD active surface area. The aim of the present study is a nondestructive experimental determination of the MD active surface area and active volume. Methods: Ten MD dosimeters, one MD prototype, and three synthetic diamond samples were investigated in the present work. 2D maps of the MD response were recorded under scanned soft x-ray microbeam irradiation, leading to an experimental determination of the device active surface area. Profiles of the device responses were measured as well. In order to evaluate the MD active volume, the thickness of the diamond sensing layer was independently evaluated by capacitance measurements and alpha particle detection experiments. The MD sensitivity, measured at the PTW calibration laboratory, was also used to calculate the device active volume thickness. Results: An average active surface area diameter of (2.19 ± 0.02) mm was evaluated by 2D maps and response profiles of all the MDs. Average active volume thicknesses of (1.01 ± 0.13) μm and (0.97 ± 0.14) μm were derived by capacitance and sensitivity measurements, respectively. The obtained results are well in agreement with the nominal values reported in the manufacturer dosimeter specifications. A homogeneous response was observed over the whole device active area. Besides the one from the device active volume, no contributions from other components of the housing nor from encapsulation materials were observed in the 2D response maps. Conclusions: The obtained results demonstrate the high reproducibility of the MD fabrication process. The observed discrepancies among the output correction factors reported by several authors for MD response in very small fields are very unlikely to be ascribed to unintentional variations of the device active surface area and volume. It is the opinion of the authors that the role of the volume averaging as well as of other perturbation effects should be separately investigated in
doi_str_mv 10.1118/1.4961402
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A general good agreement is observed for field sizes down to about 1 cm. However, evident inconsistencies can be noticed when comparing some experimental results and Monte Carlo simulations obtained for smaller irradiation fields. This issue was tentatively attributed by some authors to unintentional large variations of the MD active surface area. The aim of the present study is a nondestructive experimental determination of the MD active surface area and active volume. Methods: Ten MD dosimeters, one MD prototype, and three synthetic diamond samples were investigated in the present work. 2D maps of the MD response were recorded under scanned soft x-ray microbeam irradiation, leading to an experimental determination of the device active surface area. Profiles of the device responses were measured as well. In order to evaluate the MD active volume, the thickness of the diamond sensing layer was independently evaluated by capacitance measurements and alpha particle detection experiments. The MD sensitivity, measured at the PTW calibration laboratory, was also used to calculate the device active volume thickness. Results: An average active surface area diameter of (2.19 ± 0.02) mm was evaluated by 2D maps and response profiles of all the MDs. Average active volume thicknesses of (1.01 ± 0.13) μm and (0.97 ± 0.14) μm were derived by capacitance and sensitivity measurements, respectively. The obtained results are well in agreement with the nominal values reported in the manufacturer dosimeter specifications. A homogeneous response was observed over the whole device active area. Besides the one from the device active volume, no contributions from other components of the housing nor from encapsulation materials were observed in the 2D response maps. Conclusions: The obtained results demonstrate the high reproducibility of the MD fabrication process. The observed discrepancies among the output correction factors reported by several authors for MD response in very small fields are very unlikely to be ascribed to unintentional variations of the device active surface area and volume. It is the opinion of the authors that the role of the volume averaging as well as of other perturbation effects should be separately investigated instead, both experimentally and by Monte Carlo simulations, in order to better clarify the behaviour of the MD response in very small fields.</description><identifier>ISSN: 0094-2405</identifier><identifier>EISSN: 2473-4209</identifier><identifier>DOI: 10.1118/1.4961402</identifier><identifier>PMID: 27587052</identifier><identifier>CODEN: MPHYA6</identifier><language>eng</language><publisher>United States: American Association of Physicists in Medicine</publisher><subject>60 APPLIED LIFE SCIENCES ; active surface area ; active volume ; Applications ; Applications of Monte Carlo methods ; Arrangements for measuring resistance, reactance, impedance, or electric characteristics derived therefrom ; Biological material, e.g. blood, urine; Haemocytometers ; Calibrating of instruments or apparatus ; calibration ; Capacitance ; capacitance measurement ; COMPUTERIZED SIMULATION ; diagnostic radiography ; Diamond ; DOSEMETERS ; Dose‐volume analysis ; dosimetry ; Dosimetry/exposure assessment ; Elemental semiconductors ; encapsulation ; IRRADIATION ; Measuring inductance or capacitance; Measuring quality factor, e.g. by using the resonance method; Measuring loss factor; Measuring dielectric constants ; microDiamond ; MONTE CARLO METHOD ; Monte Carlo methods ; Monte Carlo simulations ; Optical microscopes ; perturbation theory ; Photoelectric conversion ; RADIATION PROTECTION AND DOSIMETRY ; Radiography ; Radiometry - instrumentation ; Reproducibility of Results ; Scintigraphy ; small field dosimetry ; Soft X‐rays ; SURFACE AREA ; Surface Properties ; synthetic diamond ; Testing or calibrating of apparatus or arrangements provided for in groups G01D1/00 to G01D15/00 ; THICKNESS ; X‐ray imaging</subject><ispartof>Medical physics (Lancaster), 2016-09, Vol.43 (9), p.5205-5212</ispartof><rights>American Association of Physicists in Medicine</rights><rights>2016 American Association of Physicists in Medicine</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c4212-24bb028a0bdd88acb9c537c4b12c9465e25f11d9a05520752c997a7544d25ab43</citedby><cites>FETCH-LOGICAL-c4212-24bb028a0bdd88acb9c537c4b12c9465e25f11d9a05520752c997a7544d25ab43</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://onlinelibrary.wiley.com/doi/pdf/10.1118%2F1.4961402$$EPDF$$P50$$Gwiley$$H</linktopdf><linktohtml>$$Uhttps://onlinelibrary.wiley.com/doi/full/10.1118%2F1.4961402$$EHTML$$P50$$Gwiley$$H</linktohtml><link.rule.ids>230,314,776,780,881,1411,27901,27902,45550,45551</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/27587052$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink><backlink>$$Uhttps://www.osti.gov/biblio/22689290$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Marinelli, Marco</creatorcontrib><creatorcontrib>Prestopino, G.</creatorcontrib><creatorcontrib>Verona, C.</creatorcontrib><creatorcontrib>Verona-Rinati, G.</creatorcontrib><title>Experimental determination of the PTW 60019 microDiamond dosimeter active area and volume</title><title>Medical physics (Lancaster)</title><addtitle>Med Phys</addtitle><description>Purpose: Small field output correction factors have been studied by several research groups for the PTW 60019 microDiamond (MD) dosimeter, by comparing the response of such a device with both reference dosimeters and Monte Carlo simulations. A general good agreement is observed for field sizes down to about 1 cm. However, evident inconsistencies can be noticed when comparing some experimental results and Monte Carlo simulations obtained for smaller irradiation fields. This issue was tentatively attributed by some authors to unintentional large variations of the MD active surface area. The aim of the present study is a nondestructive experimental determination of the MD active surface area and active volume. Methods: Ten MD dosimeters, one MD prototype, and three synthetic diamond samples were investigated in the present work. 2D maps of the MD response were recorded under scanned soft x-ray microbeam irradiation, leading to an experimental determination of the device active surface area. Profiles of the device responses were measured as well. In order to evaluate the MD active volume, the thickness of the diamond sensing layer was independently evaluated by capacitance measurements and alpha particle detection experiments. The MD sensitivity, measured at the PTW calibration laboratory, was also used to calculate the device active volume thickness. Results: An average active surface area diameter of (2.19 ± 0.02) mm was evaluated by 2D maps and response profiles of all the MDs. Average active volume thicknesses of (1.01 ± 0.13) μm and (0.97 ± 0.14) μm were derived by capacitance and sensitivity measurements, respectively. The obtained results are well in agreement with the nominal values reported in the manufacturer dosimeter specifications. A homogeneous response was observed over the whole device active area. Besides the one from the device active volume, no contributions from other components of the housing nor from encapsulation materials were observed in the 2D response maps. Conclusions: The obtained results demonstrate the high reproducibility of the MD fabrication process. The observed discrepancies among the output correction factors reported by several authors for MD response in very small fields are very unlikely to be ascribed to unintentional variations of the device active surface area and volume. It is the opinion of the authors that the role of the volume averaging as well as of other perturbation effects should be separately investigated instead, both experimentally and by Monte Carlo simulations, in order to better clarify the behaviour of the MD response in very small fields.</description><subject>60 APPLIED LIFE SCIENCES</subject><subject>active surface area</subject><subject>active volume</subject><subject>Applications</subject><subject>Applications of Monte Carlo methods</subject><subject>Arrangements for measuring resistance, reactance, impedance, or electric characteristics derived therefrom</subject><subject>Biological material, e.g. blood, urine; Haemocytometers</subject><subject>Calibrating of instruments or apparatus</subject><subject>calibration</subject><subject>Capacitance</subject><subject>capacitance measurement</subject><subject>COMPUTERIZED SIMULATION</subject><subject>diagnostic radiography</subject><subject>Diamond</subject><subject>DOSEMETERS</subject><subject>Dose‐volume analysis</subject><subject>dosimetry</subject><subject>Dosimetry/exposure assessment</subject><subject>Elemental semiconductors</subject><subject>encapsulation</subject><subject>IRRADIATION</subject><subject>Measuring inductance or capacitance; Measuring quality factor, e.g. by using the resonance method; Measuring loss factor; Measuring dielectric constants</subject><subject>microDiamond</subject><subject>MONTE CARLO METHOD</subject><subject>Monte Carlo methods</subject><subject>Monte Carlo simulations</subject><subject>Optical microscopes</subject><subject>perturbation theory</subject><subject>Photoelectric conversion</subject><subject>RADIATION PROTECTION AND DOSIMETRY</subject><subject>Radiography</subject><subject>Radiometry - instrumentation</subject><subject>Reproducibility of Results</subject><subject>Scintigraphy</subject><subject>small field dosimetry</subject><subject>Soft X‐rays</subject><subject>SURFACE AREA</subject><subject>Surface Properties</subject><subject>synthetic diamond</subject><subject>Testing or calibrating of apparatus or arrangements provided for in groups G01D1/00 to G01D15/00</subject><subject>THICKNESS</subject><subject>X‐ray imaging</subject><issn>0094-2405</issn><issn>2473-4209</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><sourceid>EIF</sourceid><recordid>eNp90U9vFCEYBnDSaNq1eugXaEi8VJOpLwzMwLFp65-kxh5qjCfCwDspzcywHdjVfnupsxov9UQCPx7ggZAjBqeMMfWOnQrdMAF8j6y4aOtKcNDPyApAi4oLkAfkRUp3ANDUEvbJAW-lakHyFfl--XONcxhxynagHjPOY5hsDnGisaf5Fun1zTfaADBNx-DmeBHsGCdPfUxlW_HUuhy2SO2Mltqyso3DZsSX5Hlvh4SvduMh-fr-8ub8Y3X15cOn87OrygnOeLle1wFXFjrvlbKu007WrRMd406LRiKXPWNeW5CSQyvLrG5tK4XwXNpO1Ifk9ZIbUw4muZDR3bo4Teiy4bxRmmso6mRR6znebzBlM4bkcBjshHGTDFOsaWrFtCr0zULLY1OasTfrUpCdHwwD89i3YWbXd7HHu9hNN6L_K_8UXEC1gB9hwIenk8zn613g28U_PuT3N_z39CfxNs7_hK99X_8C0pShng</recordid><startdate>201609</startdate><enddate>201609</enddate><creator>Marinelli, Marco</creator><creator>Prestopino, G.</creator><creator>Verona, C.</creator><creator>Verona-Rinati, G.</creator><general>American Association of Physicists in Medicine</general><scope>CGR</scope><scope>CUY</scope><scope>CVF</scope><scope>ECM</scope><scope>EIF</scope><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope><scope>OTOTI</scope></search><sort><creationdate>201609</creationdate><title>Experimental determination of the PTW 60019 microDiamond dosimeter active area and volume</title><author>Marinelli, Marco ; Prestopino, G. ; Verona, C. ; Verona-Rinati, G.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c4212-24bb028a0bdd88acb9c537c4b12c9465e25f11d9a05520752c997a7544d25ab43</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2016</creationdate><topic>60 APPLIED LIFE SCIENCES</topic><topic>active surface area</topic><topic>active volume</topic><topic>Applications</topic><topic>Applications of Monte Carlo methods</topic><topic>Arrangements for measuring resistance, reactance, impedance, or electric characteristics derived therefrom</topic><topic>Biological material, e.g. blood, urine; Haemocytometers</topic><topic>Calibrating of instruments or apparatus</topic><topic>calibration</topic><topic>Capacitance</topic><topic>capacitance measurement</topic><topic>COMPUTERIZED SIMULATION</topic><topic>diagnostic radiography</topic><topic>Diamond</topic><topic>DOSEMETERS</topic><topic>Dose‐volume analysis</topic><topic>dosimetry</topic><topic>Dosimetry/exposure assessment</topic><topic>Elemental semiconductors</topic><topic>encapsulation</topic><topic>IRRADIATION</topic><topic>Measuring inductance or capacitance; Measuring quality factor, e.g. by using the resonance method; Measuring loss factor; Measuring dielectric constants</topic><topic>microDiamond</topic><topic>MONTE CARLO METHOD</topic><topic>Monte Carlo methods</topic><topic>Monte Carlo simulations</topic><topic>Optical microscopes</topic><topic>perturbation theory</topic><topic>Photoelectric conversion</topic><topic>RADIATION PROTECTION AND DOSIMETRY</topic><topic>Radiography</topic><topic>Radiometry - instrumentation</topic><topic>Reproducibility of Results</topic><topic>Scintigraphy</topic><topic>small field dosimetry</topic><topic>Soft X‐rays</topic><topic>SURFACE AREA</topic><topic>Surface Properties</topic><topic>synthetic diamond</topic><topic>Testing or calibrating of apparatus or arrangements provided for in groups G01D1/00 to G01D15/00</topic><topic>THICKNESS</topic><topic>X‐ray imaging</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Marinelli, Marco</creatorcontrib><creatorcontrib>Prestopino, G.</creatorcontrib><creatorcontrib>Verona, C.</creatorcontrib><creatorcontrib>Verona-Rinati, G.</creatorcontrib><collection>Medline</collection><collection>MEDLINE</collection><collection>MEDLINE (Ovid)</collection><collection>MEDLINE</collection><collection>MEDLINE</collection><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><collection>OSTI.GOV</collection><jtitle>Medical physics (Lancaster)</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Marinelli, Marco</au><au>Prestopino, G.</au><au>Verona, C.</au><au>Verona-Rinati, G.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Experimental determination of the PTW 60019 microDiamond dosimeter active area and volume</atitle><jtitle>Medical physics (Lancaster)</jtitle><addtitle>Med Phys</addtitle><date>2016-09</date><risdate>2016</risdate><volume>43</volume><issue>9</issue><spage>5205</spage><epage>5212</epage><pages>5205-5212</pages><issn>0094-2405</issn><eissn>2473-4209</eissn><coden>MPHYA6</coden><abstract>Purpose: Small field output correction factors have been studied by several research groups for the PTW 60019 microDiamond (MD) dosimeter, by comparing the response of such a device with both reference dosimeters and Monte Carlo simulations. A general good agreement is observed for field sizes down to about 1 cm. However, evident inconsistencies can be noticed when comparing some experimental results and Monte Carlo simulations obtained for smaller irradiation fields. This issue was tentatively attributed by some authors to unintentional large variations of the MD active surface area. The aim of the present study is a nondestructive experimental determination of the MD active surface area and active volume. Methods: Ten MD dosimeters, one MD prototype, and three synthetic diamond samples were investigated in the present work. 2D maps of the MD response were recorded under scanned soft x-ray microbeam irradiation, leading to an experimental determination of the device active surface area. Profiles of the device responses were measured as well. In order to evaluate the MD active volume, the thickness of the diamond sensing layer was independently evaluated by capacitance measurements and alpha particle detection experiments. The MD sensitivity, measured at the PTW calibration laboratory, was also used to calculate the device active volume thickness. Results: An average active surface area diameter of (2.19 ± 0.02) mm was evaluated by 2D maps and response profiles of all the MDs. Average active volume thicknesses of (1.01 ± 0.13) μm and (0.97 ± 0.14) μm were derived by capacitance and sensitivity measurements, respectively. The obtained results are well in agreement with the nominal values reported in the manufacturer dosimeter specifications. A homogeneous response was observed over the whole device active area. Besides the one from the device active volume, no contributions from other components of the housing nor from encapsulation materials were observed in the 2D response maps. Conclusions: The obtained results demonstrate the high reproducibility of the MD fabrication process. The observed discrepancies among the output correction factors reported by several authors for MD response in very small fields are very unlikely to be ascribed to unintentional variations of the device active surface area and volume. It is the opinion of the authors that the role of the volume averaging as well as of other perturbation effects should be separately investigated instead, both experimentally and by Monte Carlo simulations, in order to better clarify the behaviour of the MD response in very small fields.</abstract><cop>United States</cop><pub>American Association of Physicists in Medicine</pub><pmid>27587052</pmid><doi>10.1118/1.4961402</doi><tpages>8</tpages></addata></record>
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subjects 60 APPLIED LIFE SCIENCES
active surface area
active volume
Applications
Applications of Monte Carlo methods
Arrangements for measuring resistance, reactance, impedance, or electric characteristics derived therefrom
Biological material, e.g. blood, urine
Haemocytometers
Calibrating of instruments or apparatus
calibration
Capacitance
capacitance measurement
COMPUTERIZED SIMULATION
diagnostic radiography
Diamond
DOSEMETERS
Dose‐volume analysis
dosimetry
Dosimetry/exposure assessment
Elemental semiconductors
encapsulation
IRRADIATION
Measuring inductance or capacitance
Measuring quality factor, e.g. by using the resonance method
Measuring loss factor
Measuring dielectric constants
microDiamond
MONTE CARLO METHOD
Monte Carlo methods
Monte Carlo simulations
Optical microscopes
perturbation theory
Photoelectric conversion
RADIATION PROTECTION AND DOSIMETRY
Radiography
Radiometry - instrumentation
Reproducibility of Results
Scintigraphy
small field dosimetry
Soft X‐rays
SURFACE AREA
Surface Properties
synthetic diamond
Testing or calibrating of apparatus or arrangements provided for in groups G01D1/00 to G01D15/00
THICKNESS
X‐ray imaging
title Experimental determination of the PTW 60019 microDiamond dosimeter active area and volume
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