US2022128464A1PendingUtilityA1
Refractive-index sensor and method
Assignee: THE ADMINISTRATORS OF THE TULANE EDUCATIONAL FUNDPriority: May 15, 2018Filed: Jan 3, 2022Published: Apr 28, 2022
Est. expiryMay 15, 2038(~11.8 yrs left)· nominal 20-yr term from priority
G02B 1/005G01N 21/4133B82Y 15/00G02B 1/002B82Y 20/00
60
PatentIndex Score
0
Cited by
0
References
0
Claims
Abstract
A method for measuring a refractive index of a medium includes exciting a first antisymmetric resonance of a first metasurface, including a first periodic array of resonators formed on a substrate surface, with illumination incident on the first metasurface at a non-normal incidence angle with respect to the substrate surface, the first metasurface including the medium encapsulating the first periodic array of resonators. The method also includes determining a refractive index of the medium from a first amplitude of a first transmitted signal that includes a portion of the illumination transmitted through the first metasurface.
Claims
exact text as granted — not AI-modifiedWhat is claimed is:
1 . A method for measuring a refractive index of a medium, comprising:
exciting a first anti symmetric resonance of a first metasurface, including a first periodic array of resonators formed on a substrate surface, with illumination incident on the first metasurface at a non-normal incidence angle with respect to the substrate surface, the first metasurface including the medium encapsulating the first periodic array of resonators; and determining a refractive index of the medium from a first amplitude of a first transmitted signal that includes a portion of the illumination transmitted through the first metasurface.
2 . The method of claim 1 , a spectrum of the first transmitted signal having a stopband at a center wavelength λ 1 with a linewidth δλ 1 , center wavelength λ 1 exceeding both a maximum spatial dimension of each resonator of the first periodic array of resonators and a unit cell size of the first periodic array, wherein, when the illumination has a spectral bandwidth exceeding linewidth δλ 1 and including center wavelength λ 1 , determining the refractive index comprising:
determining center wavelength λ 1 from the first transmitted signal; and
determining the refractive index at center wavelength λ 1 according to a lookup table that maps each of a plurality of stopband center-wavelengths to a respective one of a plurality of candidate refractive indices of the medium.
3 . The method of claim 1 , a spectrum of the first transmitted signal having a stopband with a linewidth δλ 1 wherein, when the illumination has a center wavelength λ 0 and a spectral bandwidth less than linewidth δλ 1 , determining the refractive index comprising:
determining the refractive index from the first transmitted signal according to a lookup table that maps each of a plurality of numerically-simulated transmittances of the medium, at center wavelength λ 0 , to a respective one of a plurality of refractive indices of the medium.
4 . The method of claim 1 , when exciting the first antisymmetric resonance, the non-normal incidence angle being between two degrees and ten degrees.
5 . The method of claim 1 , further comprising:
exciting, with the illumination, a second antisymmetric resonance of a second metasurface including a second periodic array of resonators formed on a substrate surface, the second periodic array geometrically differing from the first periodic array; and determining the refractive index of the medium from a second amplitude of a second transmitted signal and the first amplitude, the second transmitted signal including a portion of the illumination transmitted through the second metasurface.
6 . The method of claim 1 , further comprising:
exciting, with the illumination, a second antisymmetric resonance of a second metasurface including a second periodic array of resonators formed on a substrate surface, the second periodic array geometrically differing from the first periodic array; and determining whether a change in the first amplitude is caused by a change in center wavelength of the illumination or a change in the refractive index of the medium by comparing the change in the first amplitude to a change in a second amplitude of a second transmitted signal, the second transmitted signal including a portion of the illumination transmitted through the second metasurface.Cited by (0)
No later patents cite this yet.
References (0)
No backward citations on record.