{"data":{"id":"10.6084/m9.figshare.769308","type":"dois","attributes":{"doi":"10.6084/m9.figshare.769308","prefix":"10.6084","suffix":"m9.figshare.769308","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Coupe, Azaria","nameType":"Personal","givenName":"Azaria","familyName":"Coupe","affiliation":[],"nameIdentifiers":[{"schemeUri":"https://orcid.org","nameIdentifier":"https://orcid.org/0000-0003-2166-786X","nameIdentifierScheme":"ORCID"}]},{"name":"Whyntie, Tom","nameType":"Personal","givenName":"Tom","familyName":"Whyntie","affiliation":[],"nameIdentifiers":[{"schemeUri":"https://orcid.org","nameIdentifier":"https://orcid.org/0000-0003-0501-1377","nameIdentifierScheme":"ORCID"}]}],"titles":[{"title":"Strontium Decay Data"}],"publisher":"figshare","container":{},"publicationYear":2013,"subjects":[{"subject":"20203 Particle Physics","subjectScheme":"FOR"},{"subject":"FOS: Physical sciences","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"FOS: Physical sciences","subjectScheme":"Fields of Science and Technology (FOS)"}],"contributors":[],"dates":[{"date":"2013-08-12","dateType":"Created"},{"date":"2013-08-12","dateType":"Updated"},{"date":"2013","dateType":"Issued"}],"language":null,"types":{"ris":"DATA","bibtex":"misc","citeproc":"dataset","schemaOrg":"Dataset","resourceType":"Dataset","resourceTypeGeneral":"Dataset"},"relatedIdentifiers":[],"relatedItems":[],"sizes":["29581491 Bytes"],"formats":[],"version":null,"rightsList":[{"rights":"Creative Commons Attribution 4.0 International","rightsUri":"https://creativecommons.org/licenses/by/4.0/legalcode","schemeUri":"https://spdx.org/licenses/","rightsIdentifier":"cc-by-4.0","rightsIdentifierScheme":"SPDX"}],"descriptions":[{"description":"Data taken with Timepix hybrid silicon detector to measure the attenuation of beta particles from Strontium-90 in Aluminium of varying thickness. Detector settings can be found in .dsc files alongside data. Distance from source to detector = 9.3cm, Distance from source to Aluminium = 4cm. Inside the zip file, the data for each thickness of aluminium is saved in a file with the thickness as its filename. Data is stored in data.txt files in X,Y,C format, where X is the x-co-ordinate of the hit pixel in the Timepix detector's 256x256 pixel silicon sensor element, Y is the y-co-ordinate of the pixel, and C is the number of counts recorded in the pixel. The counts recorded is equivalent to the charge deposited in the pixel about a predetermined threshold value. The detector is run in Time Over Threshold mode, where it measures the charge for the amount of time it is above the threshold value.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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","url":"https://figshare.com/articles/dataset/Strontium_Decay_Data/769308","contentUrl":null,"metadataVersion":6,"schemaVersion":"http://datacite.org/schema/kernel-4","source":"mds","isActive":true,"state":"findable","reason":null,"viewCount":0,"viewsOverTime":[],"downloadCount":0,"downloadsOverTime":[],"referenceCount":0,"citationCount":0,"citationsOverTime":[],"partCount":0,"partOfCount":0,"versionCount":0,"versionOfCount":0,"created":"2013-08-12T15:40:24.000Z","registered":"2013-08-12T15:40:25.000Z","published":"2013","updated":"2020-09-05T01:36:18.000Z"},"relationships":{"client":{"data":{"id":"figshare.ars","type":"clients"}},"provider":{"data":{"id":"otjm","type":"providers"}},"media":{"data":{"id":"10.6084/m9.figshare.769308","type":"media"}},"references":{"data":[]},"citations":{"data":[]},"parts":{"data":[]},"partOf":{"data":[]},"versions":{"data":[]},"versionOf":{"data":[]}}}}