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Volumn 73, Issue 2, 2005, Pages 127-140

Interference with correlated photons: Five quantum mechanics experiments for undergraduates

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EID: 26944461177     PISSN: 00029505     EISSN: None     Source Type: Journal    
DOI: 10.1119/1.1796811     Document Type: Article
Times cited : (125)

References (35)
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    • Since we completed this work, the available power levels for the 400-410 nm diode lasers have risen to 50 mW. In addition, new diode lasers at 375 nm have become available.
    • Since we completed this work, the available power levels for the 400-410 nm diode lasers have risen to 50 mW. In addition, new diode lasers at 375 nm have become available.
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    • If the initial propagation direction is (1,0,0), with polarization along (0,0,1), then a sequence of mirrors that send the beam consecutively through the directions (0,0,1), (0,1,0), (1,0,0) rotates the polarization by 90°. Omitting the last step allows the same rotation when steering the beam into the (0,1,0) direction.
    • If the initial propagation direction is (1,0,0), with polarization along (0,0,1), then a sequence of mirrors that send the beam consecutively through the directions (0,0,1), (0,1,0), (1,0,0) rotates the polarization by 90°. Omitting the last step allows the same rotation when steering the beam into the (0,1,0) direction.
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    • In this case the π/2 relative phase between r and t yields P(δ) = 2RT[1 - cos δ].
    • In this case the π/2 relative phase between r and t yields P(δ) = 2RT[1 - cos δ].
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    • The pattern of the maxima and minima will be the same for tagged photons as for untagged photons. A tagged photon, however, is a special case of a biphoton which is discussed later, and its pattern of partial interference is not the same as that of an untagged photon.
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    • Due to the better alignment and simpler optical arrangement that we can obtain in the experiment with collinear photons, the coincidence yield is much higher than in the experiments with the noncollinear photons
    • Due to the better alignment and simpler optical arrangement that we can obtain in the experiment with collinear photons, the coincidence yield is much higher than in the experiments with the noncollinear photons.
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    • Notice that the result is just the square of the result for one-photon interference. In other words, the interference pattern of the biphoton is the product of the interference patterns of single photons
    • Notice that the result is just the square of the result for one-photon interference. In other words, the interference pattern of the biphoton is the product of the interference patterns of single photons.
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    • We detect coincidences at the interferometer output by placing a beam splitter there with reflectance R' and transmittance T' and then detecting coincidences between photons leaving each output. This arrangement allows us to detect only 2R'T' of the photon pairs leaving the interferometer.
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.