Apparatus, method and system for spectrometry with a displaceable waveguide structure
US-9500827-B2 · Nov 22, 2016 · US
US10215689B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-10215689-B2 |
| Application number | US-201815874956-A |
| Country | US |
| Kind code | B2 |
| Filing date | Jan 19, 2018 |
| Priority date | Jan 26, 2017 |
| Publication date | Feb 26, 2019 |
| Grant date | Feb 26, 2019 |
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A derivative spectroscopy system for achieving a tunable resolution of 2 nm or less in resolving spectral components of an input optical signal is provided so as to estimate derivative spectra of the input optical signal based on the resolved spectral components. In the system, a first dispersive-element structure spectrally decomposes the input optical signal into subband signals. A second dispersive-element structure receives part or all of the subband signals and spectrally decomposes the received subband signals to plural spectral components. A material having a temperature-variant refractive index is used to build the second dispersive-element structure, enabling a shift of center wavelength of each spectral component as small as 2 nm of less upon changing a temperature of the second dispersive-element structure. By obtaining three spectral-component sets obtained at three different predetermined temperatures with the center-wavelength shift of 2 nm or less, first- and second-order derivative spectra are obtained with good accuracy.
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What is claimed is: 1. A derivative spectroscopy system for generating one or more derivative spectra of an input optical signal comprising: a first dispersive-element structure for spectrally decomposing the input optical signal into plural subband signals, the first dispersive-element structure comprising one or more first dispersive elements; a second dispersive-element structure for receiving one or more of the subband signals and spectrally decomposing the received one or more subband signals into a plurality of spectral components, the second dispersive-element structure comprising one or more second dispersive elements, an individual spectral component being narrower than an individual subband signal in spectral width, the individual spectral component having a center wavelength, wherein an optically transmissive material used to build the one or more second dispersive elements has a temperature-variant refractive index, and the second dispersive-element structure is configured to utilize the temperature-variant refractive index to shift the center wavelength of the individual spectral component upon a change of a temperature of the second dispersive-element structure; a heating structure for changing the temperature of the second dispersive-element structure; a plurality of optical detectors for transducing the plurality of spectral components into a plurality of intensity signals; and one or more processors configured to: estimate the one or more derivative spectra according to spectral-component sets each being the plurality of intensity signals obtained at one predetermined temperature of the second dispersive-element structure; and control the heating structure to change the second dispersive-element structure to plural predetermined temperatures one by one for obtaining the spectral-component sets. 2. The derivative spectroscopy system of claim 1 , wherein the second dispersive element is an array-waveguide grating (AWG). 3. The dispersive spectroscopy system of claim 1 , wherein the second dispersive element is an echelle grating. 4. The dispersive spectroscopy system of claim 1 , wherein the second dispersive element is an etched diffraction grating. 5. The derivative spectroscopy system of claim 1 , wherein the heating structure comprises a temperature sensor for monitoring the temperature of the second dispersive-element structure and acting as a feedback control for the heating structure. 6. The derivative spectroscopy system of claim 1 further comprising: an additional heating structure for changing a temperature of the first dispersive-element structure; wherein the one or more processors are further configured to control the additional heating structure to maintain a temperature difference between the first- and second dispersive-element structures to be within a value predetermined for reducing random disturbance in optical property of the first dispersive-element structure due to influx of heat from the second dispersive-element structure. 7. The derivative spectroscopy system of claim 1 , wherein the one or more subband signals received by the second dispersive-element structure exclude a fingerprint deficient spectrum of the input optical signal. 8. The derivative spectroscopy system of claim 7 , wherein: the first dispersive-element structure is configured to process the input optical signal having a spectral range of 1150 nm to 1550 nm in wavelength; and the fingerprint deficient spectrum has a spectral range of 1250 nm to 1350 nm in wavelength. 9. The derivative spectroscopy system of claim 1 , wherein the one or more processors are further configured to estimate a first-order derivative spectrum and a second-order derivative spectrum of the input optical signal according to three spectral-component sets obtained at three different predetermined temperatures of the second dispersive-element structure. 10. The derivative spectroscopy system of claim 1 , wherein the one or more derivative spectra include a first-order derivative spectrum and a second-order derivative spectrum, and wherein the one or more processors are further configured to: control the heating structure to change the second dispersive-element structure to the predetermined temperatures T 0 , T 1 and T 2 one by one for obtaining first, second and third spectral-component sets, wherein T 0 , T 1 and T 2 are selected such that λ T1 −λ T0 =λ T2 −λ T1 where λ T0 , λ T1 and λ T2 are center wavelengths of a same spectral component obtained at T 0 , T 1 and T 2 , respectively; and estimate values of the first- and second-order derivative spectra at λ T0 , respectively denoted as I′ T0 and I″ T0 , by I T 0 ′ = I T 1 - I T 0 λ T 1 - λ T 0 and I T 0 ″ = I T 0 + I T
Details, e.g. use of specially adapted sources, lighting or optical systems · CPC title
Modulation spectrometry; Derivative spectrometry · CPC title
the wavelengths being separated in time, e.g. through optical fibre array · CPC title
Generating the spectrum; Monochromators · CPC title
using near infrared light · CPC title
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