1982
DOI: 10.1016/s0007-8506(07)63336-8
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Infrared Two-Wavelength Interferometry for Measuring Long Length

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Cited by 6 publications
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“…Equation (8) shows that φ 1 repeats at every λ 1 /2 target displacement, while φ 2 repeats at every λ 2 /2 target displacement. For the direct acquisition of φ s = φ 2 − φ 1 which repeats at every λ s /2 target displacement, the heterodyne signal I (t) is self-multiplied by an electronic mixer or multiplier.…”
Section: Superheterodyne Detection Of φ S and Heterodyne Separation Of φmentioning
confidence: 99%
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“…Equation (8) shows that φ 1 repeats at every λ 1 /2 target displacement, while φ 2 repeats at every λ 2 /2 target displacement. For the direct acquisition of φ s = φ 2 − φ 1 which repeats at every λ s /2 target displacement, the heterodyne signal I (t) is self-multiplied by an electronic mixer or multiplier.…”
Section: Superheterodyne Detection Of φ S and Heterodyne Separation Of φmentioning
confidence: 99%
“…There were several methods for real-time phase measurement of the synthetic wavelength. One of them was to detect the phase of the synthetic wavelength in terms of the fringe contrast [7,8]. The fringe contrast was obtained by modulating the reference mirror mechanically.…”
Section: Introductionmentioning
confidence: 99%
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