2012
DOI: 10.1364/josab.29.003201
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Virtual reference interferometry: theory and experiment

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Cited by 10 publications
(11 citation statements)
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“…This leads to several pertinent purely quantumenabled features: due to the use of an energy-time entangled two-photon N 00N -state, the required precision on equilibrating the interferometer is ∼10 m instead of microns to millimetres in standard WLI [11][12][13][14]. This is particularly interesting for improving the ease-of-use as no re-alignment is necessary when changing the SUT; compared to equation 1, the third-order term d 3 n dλ 3 in equation 3 is cancelled thanks to energy-time correlations [31]; furthermore, the wavelength at which chromatic dispersion is measured, λ * , does not have to be extracted from the data, as it is exactly twice the wavelength of the continuous-wave pump laser, λ p , and can therefore be known with extremely high accuracy.…”
Section: Methodsmentioning
confidence: 99%
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“…This leads to several pertinent purely quantumenabled features: due to the use of an energy-time entangled two-photon N 00N -state, the required precision on equilibrating the interferometer is ∼10 m instead of microns to millimetres in standard WLI [11][12][13][14]. This is particularly interesting for improving the ease-of-use as no re-alignment is necessary when changing the SUT; compared to equation 1, the third-order term d 3 n dλ 3 in equation 3 is cancelled thanks to energy-time correlations [31]; furthermore, the wavelength at which chromatic dispersion is measured, λ * , does not have to be extracted from the data, as it is exactly twice the wavelength of the continuous-wave pump laser, λ p , and can therefore be known with extremely high accuracy.…”
Section: Methodsmentioning
confidence: 99%
“…the second derivative of the wavelength-dependent optical phase. Classical WLI requires, however, precise interferometer equalisation [11,12] and is influenced by third-order dispersion [13,14] which leads to systematic errors that are difficult to account for. We eliminate all those drawbacks by inferring chromatic dispersion using energy-time entangled photon pairs and coincidence counting to measure spectral correlation functions.…”
Section: Introductionmentioning
confidence: 99%
“…2(b). Note that the difference between VRI, as described in [6], and LC-VRI is the degree of imbalance between the test and reference path lengths (relative separation between the phase fronts − → U 0 and − → U 1) to allow for resolution of the interference pattern using a low resolution spectrometer. The relationship between the average period of the interference fringes and the group delay difference between the test and reference paths is given as T avg (λ 0 ) = λ 2 0 2 N g (λ 0 ) L f − L air so that the interference fringes have a larger period and can be resolved by a low resolution spectrometer when the difference is small.…”
Section: Theorymentioning
confidence: 99%
“…Recently, we introduced virtual reference interferometry (VRI) [6] to combine the single scan measurement capability of USI with the capability of BSI for characterizing first and second order chromatic dispersion directly from the interference pattern. The VRI technique in [6] used a high coherence common path interferometry configuration to characterize fibers several tens of centimeters in length without the need for a physical reference path. This setup, however, required a wide band tunable laser with a wavelength resolution of 0.1pm, which may not always be available (in the wavelength range of interest) or may be too costly in comparison to a low coherence interferometry setup.…”
Section: Introductionmentioning
confidence: 99%
“…The values are measured to be L 17 cm and β ω F 2 15 ps 2 ∕km [15] for our fiber, and the bandwidth is calculated to be 2π10.6 THz.…”
mentioning
confidence: 90%