2022
DOI: 10.1021/acsami.2c01033
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Multiphoton Nanosculpting of Optical Resonant and Nonresonant Microsensors on Fiber Tips

Abstract: This work presents a multiphoton nanosculpting process that is employed to fabricate three-dimensional (3D) mechanically assisted optical resonant and nonresonant microsensors on fiber tips. The resonant microsensor consists of a complex 3D optical cavity design with submicron resolution and advanced micromechanical features including a hinged, multipositional mirror, a 3D spring body to displace this mirror without deforming it, and adhesive-retaining features for sealing the cavity. These features represent … Show more

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Cited by 15 publications
(9 citation statements)
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“…The light injected from the fiber core interferes with the cavity, and a portion of the light will be reflected back to the fiber. If we use a broadband light source as an input and collect the reflection spectrum of the Fabry–Pérot interferometer, the wavelength of a dip of the interference pattern λ m is given by λ m = 2 n L m where n is the refractive index of the medium within the cavity, L is the length of the cavity, and m is the order of the interference dip . If the length of the cavity remains unchanged during the measurement and we always track the same order of the interference dip, L and m are constant.…”
Section: Results and Discussionmentioning
confidence: 99%
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“…The light injected from the fiber core interferes with the cavity, and a portion of the light will be reflected back to the fiber. If we use a broadband light source as an input and collect the reflection spectrum of the Fabry–Pérot interferometer, the wavelength of a dip of the interference pattern λ m is given by λ m = 2 n L m where n is the refractive index of the medium within the cavity, L is the length of the cavity, and m is the order of the interference dip . If the length of the cavity remains unchanged during the measurement and we always track the same order of the interference dip, L and m are constant.…”
Section: Results and Discussionmentioning
confidence: 99%
“…where n is the refractive index of the medium within the cavity, L is the length of the cavity, and m is the order of the interference dip. 17 If the length of the cavity remains unchanged during the measurement and we always track the same order of the interference dip, L and m are constant. By differentiating eq 2 with respect to n, we can get…”
Section: Resultsmentioning
confidence: 99%
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