{"@context":"http://iiif.io/api/presentation/2/context.json","@type":"sc:Manifest","@id":"https://iiif.quartexcollections.com/portland/iiif/8daa0b05-7e3a-4865-9329-73350132bdfb/manifest","label":"No-Go Theorem for the Composition of Quantum Systems","metadata":[{"label":"Title","value":"No-Go Theorem for the Composition of Quantum Systems"},{"label":"Collection","value":["Physics Faculty Publications"]},{"label":"Relation","value":"phy"},{"label":"Author","value":"Maximilian Schlosshauer, Arthur Fine"},{"label":"Journal Title","value":"Physical Review Letters"},{"label":"Abstract","value":"Building on the Pusey-Barrett-Rudolph theorem, we derive a no-go theorem for a vast class of deterministic hidden-variables theories, including those consistent on their targeted domain. The strength of this result throws doubt on seemingly natural assumptions (like the “preparation independence” of the Pusey-Barrett-Rudolph theorem) about how “real states” of subsystems compose for joint systems in nonentangled states. This points to constraints in modeling tensor-product states, similar to constraints demonstrated for more complex states by the Bell and Bell-Kochen-Specker theorems."},{"label":"DOI","value":"10.1103/PhysRevLett.112.070407"},{"label":"Volume","value":"112"},{"label":"Issue","value":"7"},{"label":"Publication Date","value":"D:00 M:02 Y:2014"},{"label":"Publication Information","value":"Physical Review Letters, 2014, Volume 112, Issue 7, 1-4. © 2014 American Physical Society. Archived version is the final published version."}],"description":"No-Go Theorem for the Composition of Quantum Systems","sequences":[{"@type":"sc:Sequence","canvases":[{"@id":"https://iiif.quartexcollections.com/portland/iiif/8daa0b05-7e3a-4865-9329-73350132bdfb/canvas/_1","@type":"sc:Canvas","label":"No-Go Theorem for the Composition of Quantum Systems-2","height":1651,"width":1275,"images":[{"@type":"oa:Annotation","motivation":"sc:painting","resource":{"@id":"https://iiif.quartexcollections.com/portland/iiif/9a69938f-5a66-4afc-bf75-467a003de9b7/full/full/0/default.jpg","@type":"dctypes:Image","format":"image/jpeg","service":{"@context":"http://iiif.io/api/image/2/context.json","@id":"https://iiif.quartexcollections.com/portland/iiif/9a69938f-5a66-4afc-bf75-467a003de9b7","profile":"http://iiif.io/api/image/2/level2.json","tiles":[{"width":512,"scaleFactors":[1,2,4]}]},"height":1651,"width":1275},"on":"https://iiif.quartexcollections.com/portland/iiif/8daa0b05-7e3a-4865-9329-73350132bdfb/canvas/_1","metadata":[]}],"thumbnail":{"@id":"https://iiif.quartexcollections.com/portland/iiif/9a69938f-5a66-4afc-bf75-467a003de9b7/full/500,500/0/default.jpg","@type":"dctypes:Image","height":500,"width":500}},{"@id":"https://iiif.quartexcollections.com/portland/iiif/8daa0b05-7e3a-4865-9329-73350132bdfb/canvas/_2","@type":"sc:Canvas","label":"No-Go Theorem for the Composition of Quantum Systems-3","height":1651,"width":1275,"images":[{"@type":"oa:Annotation","motivation":"sc:painting","resource":{"@id":"https://iiif.quartexcollections.com/portland/iiif/1a98dad8-3dd1-44ab-8dfe-d7efeb4cc731/full/full/0/default.jpg","@type":"dctypes:Image","format":"image/jpeg","service":{"@context":"http://iiif.io/api/image/2/context.json","@id":"https://iiif.quartexcollections.com/portland/iiif/1a98dad8-3dd1-44ab-8dfe-d7efeb4cc731","profile":"http://iiif.io/api/image/2/level2.json"},"height":1651,"width":1275},"on":"https://iiif.quartexcollections.com/portland/iiif/8daa0b05-7e3a-4865-9329-73350132bdfb/canvas/_2","metadata":[]}],"thumbnail":{"@id":"https://iiif.quartexcollections.com/portland/iiif/1a98dad8-3dd1-44ab-8dfe-d7efeb4cc731/full/500,500/0/default.jpg","@type":"dctypes:Image","height":500,"width":500}},{"@id":"https://iiif.quartexcollections.com/portland/iiif/8daa0b05-7e3a-4865-9329-73350132bdfb/canvas/_3","@type":"sc:Canvas","label":"No-Go Theorem for the Composition of Quantum Systems-4","height":1651,"width":1275,"images":[{"@type":"oa:Annotation","motivation":"sc:painting","resource":{"@id":"https://iiif.quartexcollections.com/portland/iiif/4ed4115b-43e3-4a86-b854-6db7a08c36c0/full/full/0/default.jpg","@type":"dctypes:Image","format":"image/jpeg","service":{"@context":"http://iiif.io/api/image/2/context.json","@id":"https://iiif.quartexcollections.com/portland/iiif/4ed4115b-43e3-4a86-b854-6db7a08c36c0","profile":"http://iiif.io/api/image/2/level2.json"},"height":1651,"width":1275},"on":"https://iiif.quartexcollections.com/portland/iiif/8daa0b05-7e3a-4865-9329-73350132bdfb/canvas/_3","metadata":[]}],"thumbnail":{"@id":"https://iiif.quartexcollections.com/portland/iiif/4ed4115b-43e3-4a86-b854-6db7a08c36c0/full/500,500/0/default.jpg","@type":"dctypes:Image","height":500,"width":500}},{"@id":"https://iiif.quartexcollections.com/portland/iiif/8daa0b05-7e3a-4865-9329-73350132bdfb/canvas/_4","@type":"sc:Canvas","label":"No-Go Theorem for the Composition of Quantum Systems-5","height":1651,"width":1275,"images":[{"@type":"oa:Annotation","motivation":"sc:painting","resource":{"@id":"https://iiif.quartexcollections.com/portland/iiif/7c25807f-fa1b-40fc-8ec4-9578f88fee76/full/full/0/default.jpg","@type":"dctypes:Image","format":"image/jpeg","service":{"@context":"http://iiif.io/api/image/2/context.json","@id":"https://iiif.quartexcollections.com/portland/iiif/7c25807f-fa1b-40fc-8ec4-9578f88fee76","profile":"http://iiif.io/api/image/2/level2.json"},"height":1651,"width":1275},"on":"https://iiif.quartexcollections.com/portland/iiif/8daa0b05-7e3a-4865-9329-73350132bdfb/canvas/_4","metadata":[]}],"thumbnail":{"@id":"https://iiif.quartexcollections.com/portland/iiif/7c25807f-fa1b-40fc-8ec4-9578f88fee76/full/500,500/0/default.jpg","@type":"dctypes:Image","height":500,"width":500}}]}],"thumbnail":"https://iiif.quartexcollections.com/portland/iiif/9a69938f-5a66-4afc-bf75-467a003de9b7/full/300,300/0/default.jpg","logo":"https://iiif.quartexcollections.com/portland/iiif/logo"}