{"?xml":{"@version":"1.0"},"edm:RDF":{"@xmlns:dc":"http://purl.org/dc/elements/1.1/","@xmlns:edm":"http://www.europeana.eu/schemas/edm/","@xmlns:wgs84_pos":"http://www.w3.org/2003/01/geo/wgs84_pos","@xmlns:foaf":"http://xmlns.com/foaf/0.1/","@xmlns:rdaGr2":"http://rdvocab.info/ElementsGr2","@xmlns:oai":"http://www.openarchives.org/OAI/2.0/","@xmlns:owl":"http://www.w3.org/2002/07/owl#","@xmlns:rdf":"http://www.w3.org/1999/02/22-rdf-syntax-ns#","@xmlns:ore":"http://www.openarchives.org/ore/terms/","@xmlns:skos":"http://www.w3.org/2004/02/skos/core#","@xmlns:dcterms":"http://purl.org/dc/terms/","edm:WebResource":[{"@rdf:about":"http://www.dlib.si/stream/URN:NBN:SI:doc-ICBG5F3B/c0ada084363a9-b40-70c293a7-a08-cb6f0/PDF","dcterms:extent":"1488 KB"},{"@rdf:about":"http://www.dlib.si/stream/URN:NBN:SI:doc-ICBG5F3B/f1516281-1b90-4dfd-9cab-9955519cd1e6/TEXT","dcterms:extent":"30 KB"}],"edm:TimeSpan":{"@rdf:about":"2014-2024","edm:begin":{"@xml:lang":"en","#text":"2014"},"edm:end":{"@xml:lang":"en","#text":"2024"}},"edm:ProvidedCHO":{"@rdf:about":"URN:NBN:SI:doc-ICBG5F3B","dcterms:isPartOf":[{"@rdf:resource":"https://www.dlib.si/details/URN:NBN:SI:spr-OE00UKYR"},{"@xml:lang":"sl","#text":"Matrika"}],"dcterms:issued":"2023","dc:creator":"Kotnik, Maša","dc:format":[{"@xml:lang":"sl","#text":"letnik:10"},{"@xml:lang":"sl","#text":"13 str."},{"@xml:lang":"sl","#text":"številka:2"}],"dc:identifier":["COBISSID_HOST:166304771","ISSN:2385-8567","URN:URN:NBN:SI:doc-ICBG5F3B"],"dc:language":"sl","dc:publisher":{"@xml:lang":"sl","#text":"Založba Fakultete za matematiko in fiziko Univerze v Ljubljani"},"dc:subject":[{"@xml:lang":"en","#text":"Feynman path integral"},{"@xml:lang":"sl","#text":"Feynmanov integral po poti"},{"@xml:lang":"sl","#text":"kvantna mehanika"},{"@xml:lang":"sl","#text":"Lagrangev formalizem"},{"@xml:lang":"en","#text":"Lagrangian formalism"},{"@xml:lang":"en","#text":"quantum mechanics"}],"dcterms:temporal":{"@rdf:resource":"2014-2024"},"dc:title":{"@xml:lang":"sl","#text":"Feynmanov integral po poti|"},"dc:description":[{"@xml:lang":"sl","#text":"The article delves into the fundamental concepts of Feynman’s formulation of quantum mechanics, often neglected due to time constraints in the undergraduate physics course. Beginning with the well-known double-slit experiment and drawing inspiration from classical mechanics, it introduces the Lagrangian formalism for quantum systems. Furthermore, the article demonstrates the equivalence between Feynman and Schrödinger interpretation of quantum mechanics by deriving the Schrödinger equation from the path integral"},{"@xml:lang":"sl","#text":"V članku so obravnavani osrednji koncepti Feynmanove formulacije kvantne mehanike, za katere na dodiplomskem študiju fizike občasno zmanjka časa. Izhajajoč iz dobro poznanega poskusa z dvojno režo je po zgledu iz klasične mehanike predstavljen Lagrangev formalizem za kvantne sisteme. Na koncu je prikazana ekvivalenca med Feynmanovo in Schrödingerjevo sliko z izpeljavo Schrödingerjeve enačbe iz popotnega integrala"}],"edm:type":"TEXT","dc:type":[{"@xml:lang":"sl","#text":"znanstveno časopisje"},{"@xml:lang":"en","#text":"journals"},{"@rdf:resource":"http://www.wikidata.org/entity/Q361785"}]},"ore:Aggregation":{"@rdf:about":"http://www.dlib.si/?URN=URN:NBN:SI:doc-ICBG5F3B","edm:aggregatedCHO":{"@rdf:resource":"URN:NBN:SI:doc-ICBG5F3B"},"edm:isShownBy":{"@rdf:resource":"http://www.dlib.si/stream/URN:NBN:SI:doc-ICBG5F3B/c0ada084363a9-b40-70c293a7-a08-cb6f0/PDF"},"edm:rights":{"@rdf:resource":"http://rightsstatements.org/vocab/InC/1.0/"},"edm:provider":"Slovenian National E-content Aggregator","edm:dataProvider":{"@xml:lang":"en","#text":"National and University Library of Slovenia"},"edm:object":{"@rdf:resource":"http://www.dlib.si/streamdb/URN:NBN:SI:doc-ICBG5F3B/maxi/edm"},"edm:isShownAt":{"@rdf:resource":"http://www.dlib.si/details/URN:NBN:SI:doc-ICBG5F3B"}}}}