{"data":{"id":"10.4121/14914806","type":"dois","attributes":{"doi":"10.4121/14914806","prefix":"10.4121","suffix":"14914806","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Avis, Guus","nameType":"Personal","givenName":"Guus","familyName":"Avis","nameIdentifiers":[{"nameIdentifier":"0000-0001-7035-8065","nameIdentifierScheme":"https://orcid.org/"}],"affiliation":[]},{"name":"Rabbie, Julian","givenName":"Julian","familyName":"Rabbie","affiliation":[],"nameIdentifiers":[]},{"name":"Wehner, S.D.C. (Stephanie)","nameType":"Personal","givenName":"S.D.C. (Stephanie)","familyName":"Wehner","nameIdentifiers":[{"nameIdentifier":"0000-0002-8433-0730","nameIdentifierScheme":"https://orcid.org/"}],"affiliation":[]},{"name":"Chakraborty, Kaushik","nameType":"Personal","givenName":"Kaushik","familyName":"Chakraborty","nameIdentifiers":[{"nameIdentifier":"0000-0002-6425-0418","nameIdentifierScheme":"https://orcid.org/"}],"affiliation":[]}],"titles":[{"title":"Data for paper Designing Quantum Networks Using Preexisting Infrastructure"}],"publisher":"4TU.ResearchData","container":{},"publicationYear":2021,"subjects":[{"subject":"Quantum Physics","subjectScheme":"Australian and New Zealand Standard Research Classification (ANZSRC), 2008","classificationCode":"0206"},{"subject":"FOS: Physical sciences","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"Communication Networks and Services","subjectScheme":"Australian and New Zealand Standard Research Classification (ANZSRC), 2008","classificationCode":"8901"},{"subject":"Communications Technologies","subjectScheme":"Australian and New Zealand Standard Research Classification (ANZSRC), 2008","classificationCode":"1005"},{"subject":"quantum repeater"},{"subject":"integer linear programming"},{"subject":"repeater allocation problem"},{"subject":"quantum network"},{"subject":"designing quantum networks"}],"contributors":[{"name":"QuTech, Delft University Of Technology","nameType":"Organizational","affiliation":[],"contributorType":"Other","nameIdentifiers":[]},{"name":"Kavli Institute Of Nanoscience, Delft University Of Technology","nameType":"Organizational","affiliation":[],"contributorType":"Other","nameIdentifiers":[]}],"dates":[{"date":"2021-07-13","dateType":"Issued"}],"language":null,"types":{"ris":"DATA","bibtex":"misc","citeproc":"dataset","schemaOrg":"Dataset","resourceType":"Dataset","resourceTypeGeneral":"Dataset"},"relatedIdentifiers":[{"relationType":"References","relatedIdentifier":"https://arxiv.org/abs/2005.14715","relatedIdentifierType":"URL"}],"relatedItems":[],"sizes":[],"formats":[],"version":"1","rightsList":[{"rights":"Creative Commons Zero v1.0 Universal","rightsUri":"https://creativecommons.org/publicdomain/zero/1.0/legalcode","schemeUri":"https://spdx.org/licenses/","rightsIdentifier":"cc0-1.0","rightsIdentifierScheme":"SPDX"}],"descriptions":[{"description":"This is the data corresponding to the paper Designing Quantum Networks Using Preexisting Infrastructure. It contains data for parameter scans over different parameters that go into our method for solving the Repeater Allocation Problem and for the computation duration as a function of network size. In both cases, sample networks were generated as random geometric graphs. More information about the methodology can be found in the paper.\u003cbr\u003eAll data is in CSV format. Additionally, one python file is included that can be used to create plots based on the parameter-scan data (i.e. scan_D-(...).csv, scan_Lmax-(...).csv and scan_K-(...).csv).\u003cbr\u003e\u003cbr\u003eThe python code used to generate the data can be found in the this GitHub repository: https://github.com/jtrabbie/RepAlloc .\u003cbr\u003e","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[{"awardTitle":"Quantum Internet Alliance","funderName":"European Commission","awardNumber":"820445"},{"awardTitle":"Quantum Software Consortium","funderName":"Netherlands Organisation for Scientific Research","awardNumber":"024.003.037"}],"xml":"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