{"created":"2023-05-15T14:56:42.003446+00:00","id":76948,"links":{},"metadata":{"_buckets":{"deposit":"8f4c48ed-25a0-4eca-ac49-e363b0283d6c"},"_deposit":{"created_by":1,"id":"76948","owners":[1],"pid":{"revision_id":0,"type":"depid","value":"76948"},"status":"published"},"_oai":{"id":"oai:repo.qst.go.jp:00076948","sets":["10:29"]},"author_link":["786587","786586","786583","786581","786585","786582","786589","786588","786584"],"item_10005_date_7":{"attribute_name":"発表年月日","attribute_value_mlt":[{"subitem_date_issued_datetime":"2019-09-20","subitem_date_issued_type":"Issued"}]},"item_10005_description_5":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"Background and Objectives\nRecently, radiation therapies have been recognized as effective candidates for the cancer treatment. Among them, the targeted radioimmunotherapy using radiolabeled copper (Ⅱ) (diacetyl-bis N4-methylthiosemicarbazone) (64Cu-ATSM) is underdevelopment as a new generational cancer treatment 1). 64Cu decays by emission of β- (0.573 MeV), β+ (0.656 MeV) and electron capture (41%) with half-life of 12.7 h. The specific feature of 64Cu is the emission of auger electrons, which has been expected to be effective to kill cancer cells. The therapeutic effectiveness of 64Cu-ATSM for hypoxic cancer cells has been demonstrated so far but the absorbed dose from 64Cu has not been quantitatively evaluated. To establish a dose evaluation method of electrons, we, in the first step, have conducted the dosimetry of 64Cu. \n\nExperiments\nFluorescence Nuclear Track Detector (FNTD) (Landauer, Ltd.) with a thickness of 90 μm was employed for the dosimetry. The fluorescence intensities were measured using confocal laser scanning microscope (FV-1000, Olympus Co.). FNTD was excited by a laser with a wavelength of 635 nm and then we read the luminescence intensity at 668 nm.\nAn aqueous copper nitrate solution (FUJIFILM), which was labeled by 64Cu, was used as an electrons source. The radioactivity was 684 kBq at 10:30 on December 20th, 2018. We removed aqueous copper nitrate solution at 13:00 on January 28th, 2019. \n\nResults and Discussion\nFigure 1 shows the depth dependence of relative fluorescence intensity, that is proportional to the absorbed dose. Inset photos are confocal microscopic images of FNTD. The fluorescence intensity at deeper layer could be darker due to the optical light absorption of both excited and emitted lights. The changes in the intensity are calibrated by gamma exposures. The relative intensity decreases monotonically with increasing the depth. At 0 μm in depth, the high absorbed dose is predominantly attributed to auger electrons, characteristic X-rays, β- and β+. Furthermore, the continuous slowing down approximation range of β- in FNTD is 0.85 cm calculated by E-STAR program2). This implies that we should consider the influence to the normal tissues by β- and β+.\n\nConclusion\nWe clarified depth dependence of fluorescence intensity measured by FNTD. We are addressing to evaluate the 60Co equivalent dose in water at each depth. Additionally, the results obtained present work will be compared to that using a Monte Carlo simulation.\n","subitem_description_type":"Abstract"}]},"item_10005_description_6":{"attribute_name":"会議概要（会議名, 開催地, 会期, 主催者等）","attribute_value_mlt":[{"subitem_description":"19th International Conference on Solid State Dosimetry","subitem_description_type":"Other"}]},"item_access_right":{"attribute_name":"アクセス権","attribute_value_mlt":[{"subitem_access_right":"metadata only access","subitem_access_right_uri":"http://purl.org/coar/access_right/c_14cb"}]},"item_creator":{"attribute_name":"著者","attribute_type":"creator","attribute_value_mlt":[{"creatorNames":[{"creatorName":"楠本, 多聞"}],"nameIdentifiers":[{"nameIdentifier":"786581","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"小平聡"}],"nameIdentifiers":[{"nameIdentifier":"786582","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Fromm, Michel"}],"nameIdentifiers":[{"nameIdentifier":"786583","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Omar, Norhan"}],"nameIdentifiers":[{"nameIdentifier":"786584","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"長谷川純崇"}],"nameIdentifiers":[{"nameIdentifier":"786585","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"小川原亮"}],"nameIdentifiers":[{"nameIdentifier":"786586","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"小西輝昭"}],"nameIdentifiers":[{"nameIdentifier":"786587","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"甲斐健師"}],"nameIdentifiers":[{"nameIdentifier":"786588","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Kusumoto, Tamon","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"786589","nameIdentifierScheme":"WEKO"}]}]},"item_language":{"attribute_name":"言語","attribute_value_mlt":[{"subitem_language":"eng"}]},"item_resource_type":{"attribute_name":"資源タイプ","attribute_value_mlt":[{"resourcetype":"conference object","resourceuri":"http://purl.org/coar/resource_type/c_c94f"}]},"item_title":"Dose estimation of electrons and positrons from 64Cu using fluorescence nuclear track detector","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"Dose estimation of electrons and positrons from 64Cu using fluorescence nuclear track detector"}]},"item_type_id":"10005","owner":"1","path":["29"],"pubdate":{"attribute_name":"公開日","attribute_value":"2019-09-27"},"publish_date":"2019-09-27","publish_status":"0","recid":"76948","relation_version_is_last":true,"title":["Dose estimation of electrons and positrons from 64Cu using fluorescence nuclear track detector"],"weko_creator_id":"1","weko_shared_id":-1},"updated":"2023-05-16T00:08:27.712969+00:00"}