Methods and apparatus for spectrometry using multimode interference in a tapered spiral-shaped waveguide
Multimode interference can be used to achieve ultra-high resolving powers (e.g., Q>10 5 ) with linewidths down to 10 pm at 1500 nm and a broad spectroscopy range (e.g., 400-2400 nm) within a monolithic, millimeter-scale device. For instance, multimode interference (MMI) in a tapered waveguide enables fine resolution and broadband spectroscopy in a compact, monolithic device. The operating range is limited by the transparency of the waveguide material and the sensitivity of the camera; thus, the technique can be easily extended into the ultraviolet and mid- and deep-infrared spectrum. Experiments show that a tapered fiber multimode interference spectrometer can operate across a range from 500 nm to 1600 nm (B=1.0576) without moving parts. The technique is suitable for on-chip tapered multimode waveguides, which could be fabricated in high volume by printing or optical lithography, for applications from biochemical sensing to the life and physical sciences.
1. A spectrometer comprising:
an integrated multimode waveguide to guide at least two spatial modes of an electromagnetic beam along a propagation axis, the integrated multimode waveguide comprising a tapered spiral-shaped portion defining a dispersive region having an intermodal dispersion that varies as a function of position along the propagation axis;
a detector array, in optical communication with the dispersive region of the integrated multimode waveguide, to image an interference pattern produced by at least a portion of the at least two spatial modes of the electromagnetic beam; and
a processor, operably coupled to the detector array, to estimate a spectrum of the electromagnetic beam based at least in part on the interference pattern sensed by the detector array.
2. The spectrometer of claim 1 , wherein:
the integrated multimode waveguide comprises a layer of dielectric material having a first refractive index disposed on another material having a second refractive index lower than the first refractive index, and
the detector array comprises a plurality of detector elements disposed in a plane substantially parallel to the layer of dielectric material.
3. The spectrometer of claim 1 , wherein the processor is configured to estimate the spectrum of the electromagnetic beam by computing a pseudo-inverse matrix Λ + given by a singular decomposition of a matrix Λ to obtain a least-squares solution of {right arrow over (s)}=Λ + {right arrow over (Ψ)}, where {right arrow over (s)} is an amplitude vector representing the spectrum and {right arrow over (Ψ)} is a vector representing the interference pattern.
4. The spectrometer of claim 1 , further comprising:
a memory, operably coupled to the processor, to store calibration data representative of a mapping of interference patterns of spatial modes supported by the integrated multimode waveguide to possible spectral components of the electromagnetic beam for use by the processor in determining the spectrum of the electromagnetic beam.
5. A method of sensing a spectrum of an electromagnetic beam using an integrated multimode waveguide defining a propagation direction and having a dispersive region with an intermodal dispersion that varies as a function of position along the propagation direction, the method comprising:
(A) guiding at least two spatial modes of an electromagnetic beam along the propagation direction of the integrated multimode waveguide to the dispersive region, the dispersive region having a tapered spiral-shaped portion;
(B) coupling at least a portion of the at least two spatial modes of the electromagnetic beam out of the integrated multimode waveguide via the dispersive region;
(C) sensing, with a detector array, an interference pattern produced by the at least a portion of the at least two spatial modes of the electromagnetic beam; and
(D) estimating a spectrum of the electromagnetic beam based at least in part on the interference pattern sensed by the detector array.
6. The method of claim 5 , wherein:
(A) comprises guiding the at least two spatial modes via a layer of dielectric material having a first refractive index disposed on another material having a second refractive index lower than the first refractive index, and
(C) comprises sensing the interference pattern with a plurality of detector elements disposed in a plane substantially parallel to the layer of dielectric material.
7. The method of claim 5 , wherein (D) comprises estimating the spectrum based at least in part upon calibration data representative of a mapping of interference patterns radiated by the dispersive region of the integrated multimode waveguide to possible spectral components of the electromagnetic beam.
8. The method of claim 5 , wherein (D) comprises computing a pseudo-inverse matrix Λ + given by a singular decomposition of a matrix Λ to obtain a least-squares solution of {right arrow over (s)}=Λ + {right arrow over (Ψ)}, where {right arrow over (s)} is an amplitude vector representing the spectrum and {right arrow over (Ψ)} is a vector representing the interference pattern.