305results about "Interferometric spectrometry" patented technology

A platform for characterizing biomolecules, biological tissue sections, viruses, or other particles of interest in a non-invasive, high-throughput, cost-effective, and label-free manner. The platform includes a merged set of imaging modalities including and capable of interferometric microscopy and wide-field or confocal microscopy (such as, for example, a wide-field super-resolution surface enhanced Raman spectroscopy, SERS), although some aspects may be employed with data sets only received from wide-field or confocal microscopy. Related devices, systems, methods, techniques, and variations to the same are also provided.

Aspects relate to a compact and low-cost gas analyzer that can be used for different types of gas analysis, such as air quality analysis. The gas analyzer can include a light source, a gas cell configured to receive a sample (e.g., a gas under test), a spectral sensor including a spectrometer and a detector, and an artificial intelligence (AI) engine. Light can enter the gas cell and interact with the sample to produce output light that may be measured by the spectral sensor. The resulting spectrum produced by the spectral sensor may be analyzed by the AI engine to produce a result. The gas analyzer further includes a self-calibration component configured to enable calibration of the sample spectrum to compensate for spectral drift of the spectral sensor.

The utility model discloses an ultrafast space-time light field measuring system, which performs dispersion separation on an interference light field generated after superposition of a laser pulse to be measured and a reference pulse, and performs wavelength screening on the interference light field after dispersion separation by using a wavelength screening element to obtain a laser light field with a target wavelength. Acquiring light field complex amplitude information corresponding to the laser light field of the target wavelength; and reconstructing according to the light field complex amplitude information to obtain a light field corresponding to the laser pulse to be measured. According to the system disclosed by the utility model, the delay between the signal light and the reference light in the measured laser pulse does not need to be regulated and controlled, and the ultrafast space-time light field can be reconstructed only by enabling the same-frequency components to interfere in the same spatial position to obtain the interference pattern of each frequency. The system provided by the utility model has the characteristics of convenience in implementation, interference resistance, low background noise, low data volume, high measurement efficiency and high measurement result accuracy.

Provided are a laser interferometer capable of reducing the frequency of a signal calculated and processed in a demodulation circuit and reducing the cost of the demodulation circuit, and a spectroscopic device provided with the laser interferometer. A laser interferometer is provided with: an optical modulator that adds a modulation signal to laser light using a resonator element; a light receiving element that detects a change in the intensity of the laser light including the sampled signal and the modulated signal, and outputs a laser reception signal; a signal oscillation unit that generates a reference signal of a first frequency with the vibration element as a source vibration; and a demodulation circuit that demodulates the sampled signal from the laser reception signal on the basis of the reference signal, the demodulation circuit comprising: a DC offset removal unit that removes the offset; a first phase regulator that regulates the phase of the reference signal; a first multiplier that multiplies the laser reception signal by a reference signal; a first filter; a second multiplier multiplying the first multiplication signal by a reference signal; a second filter; and a phase calculator that calculates a phase.

The invention provides Fourier transform spectrum equipment based on phase regulation and control and a spectrum detection method, and relates to the technical field of spectrum measurement. The Fourier transform spectrum equipment comprises a light source module used for providing detection light; the spectroscope is used for splitting the detection light into first scanning light and first reference light; the scanning module is used for introducing phase delay linearly related to the light frequency into the first scanning light to obtain second scanning light, and providing the second scanning light for the sample through the spectroscope; the reference module is used for reflecting the first reference light to obtain second reference light and providing the second reference light for the sample through the spectroscope; the photoelectric detector is used for receiving the second scanning light acted on the sample and the second reference light acted on the sample to obtain a first interference pattern; and the processing module is used for processing the first interference spectrum to obtain a spectrum detection result of the sample.

The invention discloses a spectral interference system resolution improving method and system, and the method comprises the steps: building an ISE-Net end-to-end deep neural network model, enabling the convolution kernel size of an efficient channel attention module of the ISE-Net end-to-end deep neural network model to be adaptively determined according to the number of input channels, and constructing a mapping relation between narrowband and broadband interference signals; and generating an ideal narrowband signal and a double-bandwidth target signal according to a spectral interference physical formula, defining a loss function by minimizing deviation between model output and the target signal, updating parameters and dynamically adjusting a learning rate by using an AdamW optimizer until model loss is converged, and completing data generation and training. An input narrowband signal horizontal axis is converted to a corresponding frequency domain axis, and is subjected to time shifting and intensity scaling preprocessing to adapt to the model. A signal processing flow suitable for a single / multi-layer structure is constructed, a bandwidth expansion signal is obtained through decomposition, expansion and reconstruction, and the resolution of a spectrum interference system is improved. The method has the advantages of high calculation efficiency, high generalization and flexible deployment.

The invention discloses a one-dimensional ultra-wide field-of-view ultra-high spectral resolution dispersion coherent imaging spectrometer, which belongs to the technical field of spectral imaging, and comprises a first microlens array used for obtaining incident light of a one-dimensional ultra-wide field-of-view in a horizontal plane; the plurality of optical fibers are used for transmitting incident light of a one-dimensional ultra-wide field of view; the second micro lens array is used for collimating incident light from each optical fiber into broadband parallel light beams; the grating beam splitter interferometer is used for dispersing the broadband parallel light beams into a plurality of narrow-band parallel light beams with different propagation directions; the cylindrical lens is used for converging the two paths of coherent light of each narrow-band parallel light beam to a target block of the detector, and converging the narrow-band parallel light beams with different propagation directions to different target blocks respectively; and the detector is used for obtaining a continuous broadband ultra-high resolution spectrum according to the two paths of coherent light received by each target block. According to the invention, a one-dimensional ultra-wide field of view is obtained in a horizontal plane, and ultra-high spectral resolution can be obtained.

This invention relates to the field of optical imaging and detection technology, specifically providing a broadband snapshot-type polarization interferometry imaging detection system and method for breast tumors. A broadband light source illuminates a breast tumor tissue sample. The reflected signal light is collected and collimated by a pre-optical system, then sequentially passes through a first and a second ray shaping unit for two shearing and two polarization state transformations, resulting in two beams of linearly polarized light and two beams of circularly polarized light. These beams are imaged by an imaging lens to an area array detector to obtain a polarization interferogram, which is then demodulated to obtain all Stokes parameters of the breast tumor tissue sample. This invention achieves broadband snapshot imaging of breast tumors with all Stokes parameters without using an analyzer, doubling the light throughput compared to traditional polarization imaging instruments using analyzers. Furthermore, this invention has advantages such as compact structure, no moving parts, easy assembly and adjustment, and no need for image registration.

An aspect of the disclosure provides a non-invasive intracranial pressure sensing apparatus comprising an interferometric near infrared spectroscopy, iNIRS system, the iNIRS system comprising: a light emitting arrangement comprising: a light source configured to emit light; a sample delivery channel coupled to the light source and arranged to be coupled to the subject's scalp to direct light from the light source towards the subject's brain tissue; and a reference channel coupled to the light source for receiving light therefrom; a light detecting arrangement configured to be coupled to the subject's scalp and the light emitting arrangement, the light detecting arrangement comprising an interferometric optical detector configured to receive: (i) reference light from the reference channel, and (ii) sample light from the subject's brain, the sample light comprising light emitted from the light source; wherein the optical detector is arranged to combine the sample light with the reference light to provide combined light signals comprising one or more components at a beat frequency between sample light and reference light; and wherein the sensing apparatus comprises a controller configured to process data indicative of the combined light signals to determine an indication of intracranial blood pressure for the subject based on at least one property of a pulsatile waveform of one or more identified pulses of blood flow through the subject's brain.

Systems and methods for remote sensing in a plurality of dimensions simultaneously are provided. The plurality of dimensions include imaging, spectral sensing, and ranging at a range resolution that is orders of magnitude finer than the native time resolution of a detector used in the system.

An optical device includes: an incident optical system; an analysis optical system; and a length measurement optical system. The incident optical system includes a laser light source, and an incident light dividing element that divides the laser light. The analysis optical system includes a first light dividing element that divides the first divided light and then mixes the light, a first mirror that adds a first modulation signal to the one first divided light by movement and reflection, a second mirror, and a first light receiving element that receives the first divided light including a sample-derived signal and the first modulation signal. The length measurement optical system includes a second light dividing element that divides the second divided light and then mixes the light, an optical feedback unit that feeds back the one second divided light to the second light dividing element, and a second light receiving element that receives the second divided light including a displacement signal generated by the first mirror.

Optical device 100 comprises: separating element 102; in aspects, dispersive element 104; and optical elements 106. The separating element separates an optical signal into spectral bands, each having

The utility model relates to the technical field of optical communication, in particular to a spectrum detector and optical communication equipment. The spectrum detector comprises a double-fiber collimator used for inputting a detection light signal; the beam splitter prism is positioned on the light emitting side of the double-fiber collimator, and the light incident surface of the beam splitter prism is over against the light emitting side of the double-fiber collimator; the fixed spectroscope is positioned on one side, far away from the double-fiber collimator, of the beam splitter prism; the movable spectroscope is positioned on the reflected light emergent side of the beam splitter prism and can be close to or far away from the beam splitter prism along the light emergent direction of the beam splitter prism; the first photoelectric detector is located on the side, away from the movable spectroscope, of the beam splitter prism; the second photoelectric detector is located on the side, away from the beam splitter prism, of the fixed beam splitter. The volume of the spectrum detector can be effectively reduced.

The present disclosure provides a contact-less detection using a cross-cavity device where a small dielectric sample is placed at its center. The optical properties of the sample, such as the Kerr and Faraday rotation, or polarizability, manifest in the coupling between the cavities' electromagnetic modes and in the shift of their resonant frequencies. By calculating the dynamics of what are referred to herein as geometrical photonic states, a measuring protocol is formulated based on the quantum metric that maximizes the Fisher information and isolates the individual components of the complex dielectric function.

The invention provides an F-P spectral imaging system and method, and belongs to the technical field of spectral component measurement, and the system comprises a front lens which is used for collecting light energy and converting the light energy into emergent light meeting the limitation of the clear aperture of an F-P interferometer; the annular band optical filter comprises a central area and a plurality of concentric annular areas surrounding the central area, the bandwidth of each area is the same as the free spectral range of the F-P interferometer, and the annular band optical filter is used for eliminating level aliasing in emergent light of the front lens; the F-P interferometer is used for carrying out wavelength selection on emergent light of the annular band optical filter and outputting an interference field; the imaging mirror is used for projecting the interference field to the detector; and the detector is used for converting the projected optical signal into a digital electric signal. The F-P spectral imaging system which can maintain high spectral resolution and also can realize wide spectrum coverage is constructed by introducing the annular band optical filter which is accurately matched with the FSR of the F-P interferometer.

A method comprising at least one light source configured to generate a light of at least one wavelength and project the light over an optical path, a sample device, the device containing a sample obtained from exhalation of a person, a vortex mask configured to receive the light after the light passes through at least a portion of the sample device, the vortex mask including a series of concentric circles etched in a substrate, the vortex mask configured to provide destructive interference of coherent light received from the at least one light source, a detector configured to detect and measure wavelength intensities from the light in the optical path, the wavelength intensities being impacted by the light passing through the sample, the detector receiving the light that remained after passing through the vortex mask, and a processor configured to provide measurement results based on the wavelength intensities.

A method for linearization of photodetector response is provided that includes establishing one or more static calibration coefficients based on a comparison of a test photodetector response to a linear reference photodetector. In some examples, a dynamic calibration coefficient is determined based on an average photodetector signal. In some applications, such as FTIR, a single calibration coefficient is utilized to obtain a linearized ratio.

An optical sensor includes a substrate, a Fabry-Perot interferometer, and first and second photodetectors. The Fabry-Perot interferometer includes first and second reflectors and is mounted on the substrate such that light is transmitted through the interferometer to the substrate. The first and second photodetectors are configured to detect light transmitted through the etalon and the substrate. The first photodetector is sensitive to a first wavelength range, and the second photodetector is sensitive to a second wavelength range, wherein the first and second wavelength ranges each correspond to a different mode of the interferometer.

The invention discloses an extreme ultraviolet spectrograph calibration method based on extreme ultraviolet diffraction, and relates to the technical field of spectrograph calibration, and the technical scheme is characterized in that a desktop type XUV light source generation device is used for generating XUV light beams; a diffraction device is arranged on the propagation path of the XUV light beam, so that the XUV light beam is diffracted; taking the FID spectral line of the helium atom 2p-1s as an energy reference point, and deducing part of unknown parameters of the diffraction device and the spectrometer according to the separation distance of + / -1 level diffraction beams measured at the position corresponding to the energy; in combination with a Gaussian fitting method, the positions of 0-level light beams and + / -1-level diffraction light beams at other positions on the detector are obtained, and according to a diffraction formula, energy corresponding to all positions on the XUV spectrometer is inverted; calibration precision is ensured by correcting copper mesh placement angle deviation and CCD image angle deviation. According to the invention, XUV light is diffracted by using the copper net, and global continuous calibration of the energy axis of the spectrometer is realized by combining with a characteristic spectral line with a known wavelength.

To provide a terahertz wave interferometry device that can shorten measurement time. [Solution] The terahertz wave interference measuring device 1A comprises an optical pulse train output unit 10A, a first conversion unit 21, a second conversion unit 22, a multiplexing optical system 23, and a detection unit 40A. The optical pulse train output unit 10A outputs a periodic first optical pulse train P1 having a first repetition frequency, and a periodic second optical pulse train P2 having a second repetition frequency smaller than the first repetition frequency. The first conversion unit 21 converts the first optical pulse train P1 into a first terahertz wave T1. The second conversion unit 22 converts the second optical pulse train P2 into a second terahertz wave T2. The multiplexing optical system 23 combines the first terahertz wave T1 with the second terahertz wave T2 to generate a third terahertz wave T3. The detection unit 40A detects the third terahertz wave T3.

The present application relates to the technical field of spectral analysis, and particularly relates to a Fourier spectrometer and a control method thereof. The Fourier spectrometer provided by the present application comprises a control unit, a light receiving unit, a first detection unit, a second detection unit, an interference unit and a delay unit with a rotating structure. The second detection unit is used for sequentially inputting a laser signal to the interference unit and the delay unit to obtain a laser interference signal, and outputting the laser interference signal to the control unit to obtain a sampling clock signal, which is used for controlling the sampling frequency of the interference signal. The present application introduces the second detection unit and the delay unit with the rotating structure, so that the sampling process of the spectrometer can be more flexibly controlled, and the accuracy and efficiency of the sampling are improved. By accurately controlling the change of the optical path difference, the resolution of the spectral data is improved, which is helpful for more accurately analyzing the spectral characteristics of the sampling light.

The provided is an adjustable single-channel time-domain sampling filter, a spectrometer, and a detection method. The filter includes N stages of cascaded asymmetric interference units, where each asymmetric interference unit includes: a first waveguide splitting element, arranged at the input end, for splitting input light into two output paths; two interference arms, which respectively receive the light output from the two paths of the first waveguide splitting element and have different arm lengths; and a second waveguide splitting element, for combining the output light of the two interference arms to generate optical interference. Among the N cascaded asymmetric interference units, at least three are provided with phase modulators on their interference arms. When in use, the adjustable single-channel time-domain sampling filter tunes the phase modulators located in different cascaded asymmetric interference units to form optical channels with different spectral responses in the time sequence.

A Fourier transform spectrometer including an interferometer is provided. In one embodiment, an FT spectrometer includes an excitation light source, a beam splitter adapted to separate a metrology signal from the excitation light source and direct the metrology signal through an interferometer to a metrology detector. The FT spectrometer is additionally adapted to receive a spectral signal from the sample and pass the spectral signal through the interferometer to the spectrometer detector. The invention provides a method for correcting the movement of an interferometer reflector. In addition, a total spectroscopic method is provided that includes a spectral signal that includes Raman scattering, fluorescence, and near-infrared absorption components.

The application discloses a double-waveband Fourier transform spectrometer, and relates to the technical field of spectrometers. The spectrometer comprises a first Michelson interference optical path assembly and a second Michelson interference optical path assembly. The first Michelson interference optical path and the second Michelson optical path use the front and back surfaces of a same moving mirror as phase modulators. The coating materials of the front and back surfaces of the moving mirror are different. The reflected light beams of the front and back surfaces of the moving mirror have different wavebands. The application improves the signal quality of the spectrometer when detecting wavebands or measuring across wavebands through the double-path Michelson interference optical path assembly of the shared moving mirror.

The invention provides a high-resolution broadband integrated spectrometer based on thin film lead zirconate titanate and a preparation method, and relates to the technical field of integrated optics. The structure of the spectrometer comprises a substrate; the silicon dioxide lower cladding layer is arranged on the substrate; the lead zirconate titanate thin film waveguide layer is arranged on the silicon dioxide lower cladding, a plurality of micro-ring resonators and a plurality of array waveguide gratings are arranged in the lead zirconate titanate thin film waveguide layer, and each array waveguide grating is connected with each micro-ring resonator through a waveguide; the sectional periodic metal electrode arrangement system is arranged in each section of straight waveguide area in the micro-ring resonator; wherein the plurality of micro-ring resonators are configured with resonant wavelengths which are distributed in a staggered manner, and the interval between the adjacent resonant wavelengths is 1 / n of the interval between the array waveguide grating channels; the spectrometer is configured to change the local waveguide refractive index by using the residual polarization effect of the lead zirconate titanate thin film through a segmented polarization method so as to realize alignment of the resonant wavelength and the center of the array waveguide grating channel.

To provide a sensitivity measuring device and a sensitivity measuring method capable of measuring spectral sensitivity distribution of a light receiving element to be measured in a short time.SOLUTION: The sensitivity measurement device includes a light source, an optical system, a light collection mechanism, a position adjustment mechanism, a measurement unit, and an analysis unit. The optical system is configured to generate an interference wave by splitting light from a light source into two beams and causing the two beams to interfere with each other, and includes an optical path length difference changing mechanism configured to change an optical path length difference. The condensing mechanism condenses the interference wave at an irradiation position on the light receiving surface of the measured light receiving element. The position adjustment mechanism changes an irradiation position of the interference wave in a direction along the light receiving surface. The measurement unit controls the irradiation position and acquires a signal obtained by converting the interference wave from the light receiving element to be measured. The analysis unit calculates a component of the signal of each wavelength by Fourier transform of an interferogram obtained from the optical path length difference changed by the optical path length difference changing mechanism and the intensity of the signal measured by the measurement unit.SELECTED DRAWING: Figure 1

Provided is a Fourier transform infrared spectrophotometer having a configuration that is less likely to conduct heat from an infrared light source to an interferometer. A Fourier transform infrared spectrophotometer (100) comprises: an infrared light source (21) that emits infrared light; an interferometer (10) that includes a beam splitter, a fixed mirror, and a moving mirror, and that generates interference light from the infrared light; and a base plate (2) that has a first section (2a) where the infrared light source (21) is disposed and a second section (2b) where the interferometer (10) is disposed. The base plate (2) has a shape in which the first section (2a) and the second section (2b) form a predetermined angle.

The invention discloses a Fourier transform spectrometer system of a multiband light source structure, which comprises a multiband light source conveying unit used for transmitting light of multiple bands; the collimation unit is used for collimating the light transmitted by the multiband light source conveying unit; the light beam combining unit is used for forming a combined light beam; the light splitting unit is used for respectively transmitting and reflecting the plurality of beams of light; the reflector unit is used for receiving the multiple beams of light transmitted or reflected by the light splitting unit and retroreflecting the multiple beams of light in the incident direction of the multiple beams of light; and the detection unit is used for converging the multiple beams of light reflected by the reflector unit and receiving and detecting the converged multiple beams of light. According to the invention, input wavebands can be selected and multiple wavebands can be measured simultaneously, and near-infrared light and far-infrared light can be measured simultaneously, so that the detection efficiency is improved.

To enable an oscillation line width of a coherent light source being wavelength swept to be easily measured.SOLUTION: Light to be measured which is coherent light having been frequency swept so that an oscillation wavelength changes cyclically is generated from a frequency swept light source, and is split into a measurement part and a reference part differing in an optical path length and then multiplexed by an interference unit to obtain an interference light, which is detected by a light detection unit to obtain an interference signal. The interference signal, with a difference in optical path length of which between the measurement part and the reference part being changed, is Fourier transformed by an analysis unit, and the measured value of a noise floor value of a point image spread function for each difference in the optical path length is acquired. A measured amplitude value of a noise floor value that changes in accordance with the difference in the optical path length is calculated, an estimate coherence time is specified so that the measured amplitude value and the calculated amplitude value agree, and an oscillation line width of a coherent light source is measured on the basis of the estimate coherent time.SELECTED DRAWING: Figure 1