dc.contributorUniversidade Estadual Paulista (UNESP)
dc.creatorRomito, Alessandro
dc.date2011-05-26T19:53:35Z
dc.date2011-05-26T19:53:35Z
dc.date2011-05-26
dc.date.accessioned2017-04-05T16:58:59Z
dc.date.available2017-04-05T16:58:59Z
dc.identifierhttp://acervodigital.unesp.br/handle/123456789/4140
dc.identifierhttp://objetoseducacionais2.mec.gov.br/handle/mec/6403
dc.identifier.urihttp://repositorioslatinoamericanos.uchile.cl/handle/2250/831551
dc.descriptionConcepts of basic electromagnetic theory
dc.descriptionIn the Demonstration it is possible to choose whether to plot the charge's weak value, D2<Q2>S1(in units of the electron charge), as a function of the voltage bias (measured in μV), the phase difference, or the temperature (measured in mK). (The phase difference includes the Aharonov–Bohm flux and the phases of the transmission coefficients of both the quantum point contacts.) In all cases it is possible to control the other parameters, including the transparencies of both the quantum point contacts and the duration of the measurement (measured in nsec). In the upper panel of the Demonstration we also plot the upper bound for standard quantum average of the charge in arm 2 (the lower bound is obviously 0): the weak value is clearly beyond the marked bounds
dc.descriptionComponente Curricular::Educação Superior::Ciências Exatas e da Terra::Física
dc.relationWeakValuesInAnElectronicMachZehnderInterferometer.nbp
dc.rightsDemonstration freeware using Mathematica Player
dc.subjectWeak values in a interferometer
dc.subjectEducação Superior::Ciências Exatas e da Terra::Física::Física Clássica e Física Quântica; Mecânica e Campos
dc.subjectEducação Superior::Ciências Exatas e da Terra::Física::Eletricidade e Magnetismo; Campos e Partículas Carregadas
dc.subjectEducação Superior::Ciências Exatas e da Terra::Física::Áreas Clássicas de Fenomenologia e suas Aplicações
dc.titleWeak values in an electronic mach-zehnder interferometer
dc.typeSoftware


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