{"data":{"id":"10.15131/shef.data.3479396.v2","type":"dois","attributes":{"doi":"10.15131/shef.data.3479396.v2","prefix":"10.15131","suffix":"shef.data.3479396.v2","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Zhou, Xinxin","nameType":"Personal","givenName":"Xinxin","familyName":"Zhou","affiliation":[],"nameIdentifiers":[{"schemeUri":"https://orcid.org","nameIdentifier":"https://orcid.org/0000-0001-9022-5032","nameIdentifierScheme":"ORCID"}]},{"name":"Shiyong Zhang","affiliation":[],"nameIdentifiers":[]},{"name":"David, John","nameType":"Personal","givenName":"John","familyName":"David","affiliation":[],"nameIdentifiers":[]},{"name":"Ng, Jo Shien","nameType":"Personal","givenName":"Jo Shien","familyName":"Ng","affiliation":[],"nameIdentifiers":[]},{"name":"Tan, Chee","nameType":"Personal","givenName":"Chee","familyName":"Tan","affiliation":[],"nameIdentifiers":[]}],"titles":[{"title":"Data for paper: Avalanche breakdown characteristics of Al1-xGaxAsSb quaternary alloys"}],"publisher":"The University of Sheffield","container":{},"publicationYear":2016,"subjects":[{"subject":"90699 Electrical and Electronic Engineering not elsewhere classified","subjectScheme":"FOR"},{"subject":"FOS: Electrical engineering, electronic engineering, information engineering","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"FOS: Electrical engineering, electronic engineering, information engineering","subjectScheme":"Fields of Science and Technology (FOS)"}],"contributors":[],"dates":[{"date":"2016-08-03","dateType":"Created"},{"date":"2017-09-28","dateType":"Updated"},{"date":"2016","dateType":"Issued"}],"language":null,"types":{"ris":"DATA","bibtex":"misc","citeproc":"dataset","schemaOrg":"Dataset","resourceType":"Dataset","resourceTypeGeneral":"Dataset"},"relatedIdentifiers":[{"relationType":"IsIdenticalTo","relatedIdentifier":"10.15131/shef.data.3479396","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":["655905 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":"The files correspond to experimental results in paper: “Avalanche breakdown characteristics of Al\u003csub\u003e1-x\u003c/sub\u003eGa\u003csub\u003ex\u003c/sub\u003eAsSb quaternary alloys” DOI: 10.1109/LPT.2016.2601651. \u003cbr\u003e There are two types of files: -.PNG, which corresponds to the figures -.CSV, which are raw data in figures The work in this paper mainly focus on the experiments to accurately determine avalanche breakdown characteristics of Al\u003csub\u003e1-x\u003c/sub\u003eGa\u003csub\u003ex\u003c/sub\u003eAs\u003csub\u003e0.56\u003c/sub\u003eSb\u003csub\u003e0.44\u003c/sub\u003e for \u003ci\u003ex\u003c/i\u003e = 0 to 0.15. The test structures were p-i-n diodes with 100 nm avalanche layers to maximize usefulness of the results for high bandwidth APDs. In addition, due to a lack of experimental reports, this work included experimental confirmation of minimum bandgaps, \u003ci\u003eE\u003csub\u003eg\u003c/sub\u003e\u003c/i\u003e, of Al\u003csub\u003e1-x\u003c/sub\u003eGa\u003csub\u003ex\u003c/sub\u003eAs\u003csub\u003e0.56\u003c/sub\u003eSb\u003csub\u003e0.44\u003c/sub\u003e. The data consists of results from Al\u003csub\u003e1-x\u003c/sub\u003eGa\u003csub\u003ex\u003c/sub\u003eAs\u003csub\u003e0.56\u003c/sub\u003eSb\u003csub\u003e0.44\u003c/sub\u003e avalanche photodiodes (\u003ci\u003ex\u003c/i\u003e = 0 to 0.15): photoresponse, dark current, capacitance, bandgap, avalanche gain and breakdown voltage. More details about these data/figures can be found in README file. \u003cbr\u003e\u003cbr\u003e","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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","url":"https://figshare.shef.ac.uk/articles/dataset/Data_for_paper_Avalanche_breakdown_characteristics_of_Al1-xGaxAsSb_quater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