File:Quantum entanglement vs classical correlation video.gif
Quantum_entanglement_vs_classical_correlation_video.gif (787 × 382 pixels, file size: 15.59 MB, MIME type: image/gif, 1,000 frames, 1 min 40 s)
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[edit]DescriptionQuantum entanglement vs classical correlation video.gif |
English: This video demonstrates the difference between entangled and classically correlated quantum states when the polarization of photons is considered. In the scene on the left, the source produces photon pairs in a singlet state, which is maximally entangled. In the scene on the right, the photon pairs are created in a dephased singlet state, which is mixed and only classically correlated. In both scenes, there is a source of photon pairs in the center. One photon of each pair propagates to the detection station on the left and its partner photon propagates to the detection station on the right. Each detection station consists of a polarizing beam splitter and two detection screens. The detection stations can measure the polarization of incoming photons in different linearly-polarized bases. The video comprises three parts. In the first part, the photons are measured in the H/V basis. Both entangled and classically correlated states give rise to the same measurement results (up to random fluctuations that are intrinsic to the quantum measurements). In the second part, the measurements are performed in different bases, where the difference between the two states becomes apparent. In the third part, only the probabilities of photon detections are plotted and the detection stations are rotated smoothly over the entire range of linear polarizations. Even though the probabilities for the classically correlated state vary as the rotation angle increases, the probabilities for the entangled singlet state remain constant. Čeština: Na videu je ukázán rozdíl mezi kvantově provázanými a klasicky korelovanými kvantovými stavy fotonů. Nalevo je zobrazena scéna, kde jsou páry fotonů generovány v singletovém stavu, které je maximálně kvantově provázaný. Napravo je pak scéna, kde jsou páry ve smíšeném stavu, který odpovídá defázovanému singletovému stavu a který je jen klasicky korelovaný. Uprostřed obou scén je zdroj, který produkuje páry fotonů. Jeden foton z každého páru letí do levé měřicí stanice, druhý foton letí do stanice napravo. Obě stanice se skládají z polarizačního děliče svazku a dvou stínítek. Měřicí stanice jsou schopné měřit polarizaci v různých lineárně polarizovaných bázích. Video sestává ze tří částí. V první části jsou prováděna měření pouze v H/V bázi. V této bázi dává provázaný i klasicky korelovaný stav stejné výsledky. Ve druhé části jsou prováděna měření v různých bázích lineární polarizace. Zde je již patrný rozdíl mezi oběma stavy. V části třetí jsou zobrazeny už jen pravděpodobnosti naměření fotonu v tom kterém nastavení a měřicí stanice jsou plynule otáčeny přes celý rozsah lineárních polarizací. Zatímco pro klasicky korelovaný stav se tyto pravděpodobnosti mění pro různé úhly natočení, pravděpodobnosti pro kvantově provázaný stav zůstavají neměnné. |
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Source | Own work |
Author | JozumBjada |
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current | 15:54, 29 November 2020 | 787 × 382 (15.59 MB) | JozumBjada (talk | contribs) | Cross-wiki upload from cs.wikipedia.org |
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