CA3028758A1 - Systems and methods for interrogating parameters at a plurality of locations in a sample - Google Patents
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Classifications
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/25—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
- G01N21/31—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
- G01B9/00—Measuring instruments characterised by the use of optical techniques
- G01B9/02—Interferometers
- G01B9/02001—Interferometers characterised by controlling or generating intrinsic radiation properties
- G01B9/02007—Two or more frequencies or sources used for interferometric measurement
- G01B9/02008—Two or more frequencies or sources used for interferometric measurement by using a frequency comb
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01D—MEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
- G01D5/00—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable
- G01D5/26—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light
- G01D5/32—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light
- G01D5/34—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells
- G01D5/353—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells influencing the transmission properties of an optical fibre
- G01D5/35306—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells influencing the transmission properties of an optical fibre using an interferometer arrangement
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J3/00—Spectrometry; Spectrophotometry; Monochromators; Measuring colours
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- G01J3/45—Interferometric spectrometry
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- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/25—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
- G01N21/31—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry
- G01N21/314—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry with comparison of measurements at specific and non-specific wavelengths
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/47—Scattering, i.e. diffuse reflection
- G01N21/4795—Scattering, i.e. diffuse reflection spatially resolved investigating of object in scattering medium
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- G01N2201/00—Features of devices classified in G01N21/00
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- G01N2201/069—Supply of sources
- G01N2201/0696—Pulsed
Abstract
A system (100) for interrogating parameters at a plurality of locations in a sample (108) includes first and second ultrafast laser sources (102, 104), a reference device (110), and detector and processor units (124, 128). The first and second ultrafast laser sources (102, 104) provide first and second plurality of pulses, respectively, in a picosecond time domain or lower to interact with the sample at the plurality of locations in the sample (108) to provide processed pulses. Further, the first and second ultrafast laser sources (102 and 104) are configured to provide comb frequencies having first and second repetition rates, respectively. The detector unit (124) is configured to detect at least a portion of the processed pulses, second plurality of pulses, and referenced pulses. The processor unit (128) is configured to process the detected pulses and provide measurements of the parameters for the plurality of locations in the sample (108).
Description
SYSTEMS AND METHODS FOR INTERROGATING PARAMETERS AT A
PLURALITY OF LOCATIONS IN A SAMPLE
BACKGROUND
[0001] The embodiments of the specification relate to systems and methods for distributed measurements of one or more parameters. In particular, the systems and methods relate to the distributed measurements using optical techniques.
PLURALITY OF LOCATIONS IN A SAMPLE
BACKGROUND
[0001] The embodiments of the specification relate to systems and methods for distributed measurements of one or more parameters. In particular, the systems and methods relate to the distributed measurements using optical techniques.
[0002]
Typically, in large gas chambers or in optically transparent samples absorption of incident optical radiation is measured as a bulk quantity by passing the optical radiation through the sample. It is desirable to develop optical techniques that can provide distribution of multiple parameters such as temperature of gases, concentration of gases, and/or pressure of gases inside a chamber, or measure spatially distributed high resolution spectrum.
Typically, in large gas chambers or in optically transparent samples absorption of incident optical radiation is measured as a bulk quantity by passing the optical radiation through the sample. It is desirable to develop optical techniques that can provide distribution of multiple parameters such as temperature of gases, concentration of gases, and/or pressure of gases inside a chamber, or measure spatially distributed high resolution spectrum.
[0003] Optical frequency pulsing is an optical technique that is employed to encode information pertaining to transmission across fiber optic lines, determine physical properties of molecules in samples, and the like. Identification of sample properties using frequency pulses is based on width and stability of the pulses at desirable frequencies to obtain specific resolution of the sample. Typically, interferometric measurements are used for optical analysis of samples.
However, usually, interferometric measurements result in decreased resolution in space and time due to limitations on pulse widths, repetition rate of the pulses, range of spectra, and the like. The optical frequency pulsing for transmission of information employs relatively wide bandwidth of individual frequency pulses, resulting in overlapping pulses over large transmission distances. As will be appreciated, as frequency pulses travel along a fiberoptic line, pulse width increases. After determined distance, the overlap of frequency lines due to increase in the pulse widths results in a loss of digital information content. Further, it is difficult to generate multiple different, closely spaced frequencies, thereby limiting signal resolution in optical frequency pulsing.
BRIEF DESCRIPTION
However, usually, interferometric measurements result in decreased resolution in space and time due to limitations on pulse widths, repetition rate of the pulses, range of spectra, and the like. The optical frequency pulsing for transmission of information employs relatively wide bandwidth of individual frequency pulses, resulting in overlapping pulses over large transmission distances. As will be appreciated, as frequency pulses travel along a fiberoptic line, pulse width increases. After determined distance, the overlap of frequency lines due to increase in the pulse widths results in a loss of digital information content. Further, it is difficult to generate multiple different, closely spaced frequencies, thereby limiting signal resolution in optical frequency pulsing.
BRIEF DESCRIPTION
[0004] In one embodiment, a system for interrogating one or more parameters at a plurality of locations in a sample is provided. The system includes a first ultrafast laser source and a second ultrafast source configured to provide a first plurality of pulses and a first plurality of pulses, respectively in a picosecond time domain or lower. Further, the first and second ultrafast laser sources are configured to provide comb frequencies having first and second repetition rates, respectively, where the second repetition rate is different from the first repetition rate.
Further, the first plurality of pulses interacts with the sample at the plurality of locations in the sample to provide processed pulses. Moreover, the system includes a reference device configured to provide referenced pulses having a variable time delay, a variable phase delay, a variable path length difference, or combinations thereof Additionally, the system includes a detector unit configured to detect at least a portion of the processed pulses from the first ultrafast laser source, the second plurality of pulses from the second ultrafast laser source, and the referenced pulses.
The system also includes a processor unit configured to process the detected pulses and provide measurements of the one or more parameters for the plurality of locations in the sample.
Further, the first plurality of pulses interacts with the sample at the plurality of locations in the sample to provide processed pulses. Moreover, the system includes a reference device configured to provide referenced pulses having a variable time delay, a variable phase delay, a variable path length difference, or combinations thereof Additionally, the system includes a detector unit configured to detect at least a portion of the processed pulses from the first ultrafast laser source, the second plurality of pulses from the second ultrafast laser source, and the referenced pulses.
The system also includes a processor unit configured to process the detected pulses and provide measurements of the one or more parameters for the plurality of locations in the sample.
[0005] In another embodiment, a system for interrogating one or more parameters at a plurality of locations in a sample is provided. The system includes a first femtosecond laser source and a second femtosecond laser source configured to provide a first plurality of pulses and a first plurality of pulses, respectively, in a picosecond time domain or lower. Further, the first and second femtosecond laser sources are configured to provide comb frequencies having first and second repetition rates, respectively, where the second repetition rate is different from the first repetition rate. Further, the first plurality of pulses interacts with the sample at the plurality of locations in the sample to provide processed pulses. The system also includes a reference device configured to provide referenced pulses having a variable time delay, a variable phase delay, a variable path length difference, or combinations thereof. Further, the system includes a detector unit configured to detect at least a portion of the processed pulses from the first femtosecond laser source, the second plurality of pulses from the second femtosecond laser source, and the referenced pulses. Moreover, the system includes a processor unit configured to process the detected pulses and provide measurements of the one or more parameters for the plurality of locations in the sample.
[0006] In yet another embodiment, a method includes providing a first plurality of pulses in a picosecond time domain or lower, and comb frequencies having a first repetition rate. Further, the method includes interacting a portion of the first plurality of pulses at a plurality of locations in a sample to provide processed pulses.
The method also includes introducing a variable time delay, a variable phase delay, a variable path length difference, or combinations thereof in another portion of the first plurality of pulses to provide referenced pulses, and providing a second plurality of pulses in a picosecond time domain or lower, and comb frequencies having a second repetition rate that is different from the first repetition rate.
Additionally, the method includes detecting at least a portion of the processed pulses from the first ultrafast laser source, the second plurality of pulses from the second ultrafast laser source, and the referenced pulses. The method also includes processing the detected pulses to provide measurements of one or more parameters for the plurality of locations in the sample.
DRAWINGS
The method also includes introducing a variable time delay, a variable phase delay, a variable path length difference, or combinations thereof in another portion of the first plurality of pulses to provide referenced pulses, and providing a second plurality of pulses in a picosecond time domain or lower, and comb frequencies having a second repetition rate that is different from the first repetition rate.
Additionally, the method includes detecting at least a portion of the processed pulses from the first ultrafast laser source, the second plurality of pulses from the second ultrafast laser source, and the referenced pulses. The method also includes processing the detected pulses to provide measurements of one or more parameters for the plurality of locations in the sample.
DRAWINGS
[0007] These and other features and aspects of embodiments of the invention will become better understood when the following detailed description is read with reference to the accompanying drawings in which like characters represent like parts throughout the drawings, wherein:
[0008] FIG. 1 is a schematic representation of a system for distributed measurement of a sample to interrogate one or more parameters at a plurality of locations in the sample, in accordance with aspects of the specification;
[0009] FIGs.
2(a)-2(i) are graphical illustrations of distributed measurements using the system of FIG. 1, in accordance with aspects of the specification;
2(a)-2(i) are graphical illustrations of distributed measurements using the system of FIG. 1, in accordance with aspects of the specification;
[0010] FIG. 3 is a schematic representation of a system for long distance distributed measurements at a plurality of locations in a sample, in accordance with aspects of the specification; and
[0011] FIG. 4 is an example flow chart of a method for distributed measurements for a plurality of locations in a sample.
DETAILED DESCRIPTION
DETAILED DESCRIPTION
[0012] In certain embodiments of the specification, systems and methods for distributed measurement of one or more parameters of a sample are provided. In certain other embodiments of the specification, distributed measurement of absorption, transmission, reflection, phase spectrum, or combinations may be used to determine one or more parameters, such as, but not limited to, concentration, pressure, temperature, and chemical composition at one or more locations in the sample. Further, in some embodiments, the systems may be configured to conduct short distance distributed measurements, long distance distributed measurements, or both. In one example, the distributed measurement may be performed in the sample to determine chemical composition of the sample at two or more locations in the sample. In another embodiment, the distributed measurement may be carried out to determine temperature of the sample at two or more locations in the sample.
[0013] In some embodiments, the systems and methods may be used for high spatial resolution multi-parameter measurement along with wavelength resolution.
For example, the systems and methods may be used for spatial profiling of gas, oil, water, or combinations thereof in down hole systems, spatial gas concentration measurements, such as in a gas turbine exhaust, health monitoring of coatings, such as, but not limited to, thermal barrier coatings in turbine blades.
For example, the systems and methods may be used for spatial profiling of gas, oil, water, or combinations thereof in down hole systems, spatial gas concentration measurements, such as in a gas turbine exhaust, health monitoring of coatings, such as, but not limited to, thermal barrier coatings in turbine blades.
[0014] In certain embodiments, a system for distributed measurement of a sample to interrogate or probe one or more parameters at a plurality of locations in the sample is provided. The system includes a first ultrafast laser source configured to provide comb frequencies having a first repetition rate The first ultrafast laser source is configured to provide a first plurality of pulses in a time domain that is equal to or lower than a picosecond time domain to interact with one or more locations of the plurality of locations of the sample to provide processed pulses.
The system also includes a second ultrafast laser source that is configured to provide comb frequencies at a second repetition rate that is different from the first repetition rate. The second ultrafast laser source is configured to provide a second plurality of pulses in a time domain equal to or lower than the picosecond time domain The difference between the repetition rates of the first and second ultrafast laser sources may be based on a system parameter. Further, the difference between the repetition rates of the first and second ultrafast laser sources determines a range of spectrum that can be measured. By way of example, if the difference in the repetition rates is below a determined value, the range of spectrum that is measured may be narrower than a range of spectrum that is measured if the difference in the repetition rates is above the determined value.
The system also includes a second ultrafast laser source that is configured to provide comb frequencies at a second repetition rate that is different from the first repetition rate. The second ultrafast laser source is configured to provide a second plurality of pulses in a time domain equal to or lower than the picosecond time domain The difference between the repetition rates of the first and second ultrafast laser sources may be based on a system parameter. Further, the difference between the repetition rates of the first and second ultrafast laser sources determines a range of spectrum that can be measured. By way of example, if the difference in the repetition rates is below a determined value, the range of spectrum that is measured may be narrower than a range of spectrum that is measured if the difference in the repetition rates is above the determined value.
[0015] The system also includes a detector unit that is configured to detect at least a portion of the processed pulses and at least a portion of the second plurality of pulses. Further, the system includes a processor unit configured to process the detected pulses and provide measurements of one or more parameters corresponding to the plurality of locations in the sample.
[0016] In certain embodiments, the methods and systems may be used to provide distributed measurement of the plurality of parameters to facilitate optimization of operation, such as, but not limited to, an operation of a gas turbine.
For example, the distributed measurement of the plurality of parameters facilitate identifying hot spots in the gas turbine, reducing emissions from the gas turbine, detecting impurities in materials in thermal barrier coatings of turbine blades, and the like, or combinations thereof Further, the methods and systems may provide measurements for samples having one or more phases, such as two or more of solid, liquid, and gaseous phases. The systems and methods are configured to measure broadband high resolution spectrum and have applications in environmental studies where the samples may be in one or more phases such as solid, liquid and gaseous phases. Moreover, the methods and systems use synchronized ultrafast laser sources that facilitate long distance distributed measurements.
For example, the distributed measurement of the plurality of parameters facilitate identifying hot spots in the gas turbine, reducing emissions from the gas turbine, detecting impurities in materials in thermal barrier coatings of turbine blades, and the like, or combinations thereof Further, the methods and systems may provide measurements for samples having one or more phases, such as two or more of solid, liquid, and gaseous phases. The systems and methods are configured to measure broadband high resolution spectrum and have applications in environmental studies where the samples may be in one or more phases such as solid, liquid and gaseous phases. Moreover, the methods and systems use synchronized ultrafast laser sources that facilitate long distance distributed measurements.
[0017] FIG. 1 illustrates an example of a system for distributed measurement of a sample to interrogate one or more parameters at a plurality of locations in the sample. In the illustrated embodiment, the system 100 includes an interferometric configuration, which uses a sample arm and a reference arm. The term "sample arm" is used to refer to an arm or portion of the system 100 that includes a sample, and the term "reference arm" is used to refer to an arm or a portion of the system 100 that includes a reference device.
[0018] In the illustrated embodiment, the system 100 includes a first ultrafast laser source 102, a second ultrafast laser source 104, and a reference device 110.
The first and second ultrafast laser sources 102 and 104 are configured to provide first and second plurality of pulses, respectively. The first and second ultrafast laser sources 102 and 104 are defined by their individual frequency combs and repetition rates. The reference device 110 is operatively coupled to the first laser source 102 and configured to provide referenced pulses that have a time delay, a phase delay, or an optical path length difference with respect to the pulses of the first laser source 102.
The first and second ultrafast laser sources 102 and 104 are configured to provide first and second plurality of pulses, respectively. The first and second ultrafast laser sources 102 and 104 are defined by their individual frequency combs and repetition rates. The reference device 110 is operatively coupled to the first laser source 102 and configured to provide referenced pulses that have a time delay, a phase delay, or an optical path length difference with respect to the pulses of the first laser source 102.
[0019] In one embodiment, the difference in frequencies of the first and second ultrafast laser sources 102 and 104 may be greater than a line width of any given line of the frequency comb of the ultrafast laser sources 102 and 104.
Further, the difference in frequencies of the first and second ultrafast laser sources 102 and 104 may be less than half of the repetition rate of the ultrafast laser sources 102 and 104.
Further, the difference in frequencies of the first and second ultrafast laser sources 102 and 104 may be less than half of the repetition rate of the ultrafast laser sources 102 and 104.
[0020] In some examples, the ultrafast laser sources 102 and 104 may be pico or femtosecond laser sources. Advantageously, use of pico or femtosecond laser sources in the system 100 results in relatively higher spatial resolution as compared to use of laser sources that emit optical pulses at time durations that are greater than pico seconds. The repetition rates of the first and second ultrafast laser sources 102 and 104 are different. In one example, the repetition rate of the first ultrafast laser source 102 is referred to as the "first repetition rate," fr, and the repetition rate of the second ultrafast laser source 104 is referred to as the "second repetition rate,"
(fr +/- df). In particular, the first and second repetition rates are different. The difference in repetition rates of the first and second ultrafast laser sources 102 and 104 is represented by df, where df is a ratio that represents spatial distribution of length of laser pulses for a particular repetition rate of the ultrafast laser source.
The repetition rate may be decided based on the desirable spectral resolution.
In one embodiment, the value of df may be represented by Equation (1) as:
df = ¨c Equation (1) fr where, c represents speed of light, and fr represents repetition rate of the first ultrafast laser source 102.
(fr +/- df). In particular, the first and second repetition rates are different. The difference in repetition rates of the first and second ultrafast laser sources 102 and 104 is represented by df, where df is a ratio that represents spatial distribution of length of laser pulses for a particular repetition rate of the ultrafast laser source.
The repetition rate may be decided based on the desirable spectral resolution.
In one embodiment, the value of df may be represented by Equation (1) as:
df = ¨c Equation (1) fr where, c represents speed of light, and fr represents repetition rate of the first ultrafast laser source 102.
[0021] It may be noted that optical paths for the plurality of pulses from the ultrafast laser sources 102 and 104 may be formed with or without optical fibers.
In one embodiment, an optical fiber may be in operative communication with the first ultrafast laser source 102 such that at least a portion of the first plurality of pulses traverses through at least a portion of the optical fiber. In same or different embodiments, an optical fiber may be in operative communication with the second ultrafast laser source 104 such that at least a portion of the second plurality of pulses traverses through at least a portion of the optical fiber. In certain embodiments, in the optical configuration of FIGS. 1 and 3 of the present application, the first, second, and/or third plurality of pulses from the first, second, and/or third ultrafast laser sources 302, 304, and 306, respectively, may traverse through ambient atmosphere (e.g., air) or optical fiber. In embodiments where the different plurality of pulses traverse using the optical fiber, connecting lines between various components of the systems 100 and 300 may represent optical fibers.
In one embodiment, an optical fiber may be in operative communication with the first ultrafast laser source 102 such that at least a portion of the first plurality of pulses traverses through at least a portion of the optical fiber. In same or different embodiments, an optical fiber may be in operative communication with the second ultrafast laser source 104 such that at least a portion of the second plurality of pulses traverses through at least a portion of the optical fiber. In certain embodiments, in the optical configuration of FIGS. 1 and 3 of the present application, the first, second, and/or third plurality of pulses from the first, second, and/or third ultrafast laser sources 302, 304, and 306, respectively, may traverse through ambient atmosphere (e.g., air) or optical fiber. In embodiments where the different plurality of pulses traverse using the optical fiber, connecting lines between various components of the systems 100 and 300 may represent optical fibers.
[0022] The first ultrafast laser source 102 is operatively coupled to the reference device 110. In a non-limiting example, the reference device 110 may be a time delay device, such as a mirror. Other non-limiting examples of reference devices may include phase difference or delay generators, path length difference generators, liquid crystals, micro arrays, micro el ectro mechanical system (MEMS), or any other optical structures that are configured to introduce a time delay, a phase delay or phase difference, or an optical path length difference in a path of optical radiation in the system 100, for example. The reference arm, generally represented by reference numeral 112 includes the reference device 110, such as the reference mirror. Further, the sample arm, generally represented by reference numeral 114, includes a sample 108 and an optical path that leads to the sample 108. The reference device 110 is configured to provide a time delay between the optical pulses travelling in the reference arm 112 and the optical pulses travelling in the sample arm 114 to create a desirable interference between the pulses in the two arms 112 and 114.
[0023] In certain embodiments, the reference device may be configured to introduce a time delay, phase delay or difference, or optical path length difference, in a portion of the first plurality of pulses provided by the first ultrafast laser source 102. Further, the time delay, phase delay, or optical path length difference may be varied with time. In particular, the time delay, phase delay, path length difference, introduced by the reference device 110 in a portion of the first plurality of pulses are such that these delays and differences may be varied according to a location in the sample that is to be interrogated. By way of example, in the illustrated embodiment, if the reference device 110 is a time delay device, such as a mirror, the mirror may be configured to move along an optical path, represented by reference numeral 111, to introduce a variable time delay in the path of the portion of the first plurality of pulses from the first ultrafast laser source 102.
This portion of the first plurality of pulses is referred to as referenced pulses. Further, the speed or rate of movement of the time delay device may be adjusted based on a desirable scanning rate at which different locations of the sample 108 need to be scanned.
Further, the time delay, phase delay, or path length difference introduced by the reference device110 may be adjusted to correspond to spatial resolution of the sample 108. It may be noted that the minimal spatial resolution for scanning a sample 108 may be similar to a pulse width of the laser sources 102 and 104.
This portion of the first plurality of pulses is referred to as referenced pulses. Further, the speed or rate of movement of the time delay device may be adjusted based on a desirable scanning rate at which different locations of the sample 108 need to be scanned.
Further, the time delay, phase delay, or path length difference introduced by the reference device110 may be adjusted to correspond to spatial resolution of the sample 108. It may be noted that the minimal spatial resolution for scanning a sample 108 may be similar to a pulse width of the laser sources 102 and 104.
[0024] The system further includes splitters 116 and 117. In a non-limiting example, the splitter 116 may be a 50:50 splitter, for example. The splitter 116 is configured to split the radiation travelling from the first ultrafast laser source 102 into at least 2 portions such that a first portion of the radiation travels towards the reference device 110, and the second portion of the radiation travels towards the sample 108. Additionally, both the reference and sample arms 112 and 114 may employ collimators 120 and 122. The collimators 120 and 122 may be similar to one another in function and structure or may be different. The collimator 120 collimates and directs the radiation towards the reference device 110, the delayed radiation from the reference device 110 is received back by the collimator 120.
Similarly, the collimator 122 collimates and directs the radiation towards the sample 108 to facilitate interaction of the radiation with at least a portion of the sample 108, and to collect the processed pulses or interacted pulses.
Similarly, the collimator 122 collimates and directs the radiation towards the sample 108 to facilitate interaction of the radiation with at least a portion of the sample 108, and to collect the processed pulses or interacted pulses.
[0025] In operation, a portion of the referenced pulses, such as time delayed pulses, from the first ultrafast laser source 102 are allowed to interact with one or more locations of a sample at a given instant in time. The sample locations 130, 132, 134, and 136 are interrogated or probed based on a refractive index of a medium of the sample 108. In one example, where the reference device 110 is a time delay device, such as a reference mirror, the distance moved by the reference mirror along the optical path, which is along the direction 111 may determine an amount of optical delay or path length difference introduced in the sample arm, or both. In one embodiment, the reference mirror may be coupled to a motor (not shown in FIG. 1) to facilitate movement of the mirror. It other examples where a piezo electric device or a MEMS mirror is used as a reference device 110, electrical current may be provided to the reference device to facilitate desirable movement of the reference device 110 to provide suitable time delay or phase delay at a particular instance in time.
[0026] The interacted pulses from the sample 108 in the sample arm 114, and the referenced (such as time delayed) pulses from the reference arm 112 are allowed to interfere with the pulses from the second ultrafast laser source 104. This interference of the pulses is detected using the detector unit 124. In one example, the detector unit 124 may be a high frequency detector.
[0027] Further, the system employs a processor unit 128 for processing the combined radiation received at the detector unit 124. As used herein, the term "processor unit" refers to a processing unit having integrated circuits as being included in a computer, as well as a controller, a microcontroller, a microcomputer, a programmable logic controller (PLC), an application specific integrated circuit, application-specific processors, digital signal processors (DSPs), application specific integrated circuits (ASICs), field programmable gate arrays (FPGAs), and/or any other programmable circuits. In certain embodiments, the processor unit 128 may be coupled to, or may include a memory device(s) (not shown in FIG.
1). The memory device(s) may generally include memory element(s) including, but are not limited to, computer readable medium (e.g., random access memory (RAM)), computer readable non-volatile medium (e.g., a flash memory), one or more hard disk drives, a floppy disk, a compact disc-read only memory (CD-ROM), compact disk-read/write (CD-R/W) drives, a magneto-optical disk (MOD), a digital versatile disc (DVD), flash drives, optical drives, solid-state storage devices, and/or other suitable memory elements. The detected radiation processed by the processor unit 128 may provide data that represents distributed measurements of one or more parameters of a sample as described further in FIGS. 2(a)-2(h).
Further, the method of operation of the system 100 of FIG. 1 will be described with respect to FIGS. 2(a)-2(h).
1). The memory device(s) may generally include memory element(s) including, but are not limited to, computer readable medium (e.g., random access memory (RAM)), computer readable non-volatile medium (e.g., a flash memory), one or more hard disk drives, a floppy disk, a compact disc-read only memory (CD-ROM), compact disk-read/write (CD-R/W) drives, a magneto-optical disk (MOD), a digital versatile disc (DVD), flash drives, optical drives, solid-state storage devices, and/or other suitable memory elements. The detected radiation processed by the processor unit 128 may provide data that represents distributed measurements of one or more parameters of a sample as described further in FIGS. 2(a)-2(h).
Further, the method of operation of the system 100 of FIG. 1 will be described with respect to FIGS. 2(a)-2(h).
[0028]
Referring to FIGS. 2(a)-2(h), interference of pulses from a reference arm, for example, the reference arm 112 of FIG. 1 and a sample arm, for example, the sample arm 114 of FIG. 1 is illustrated. In FIGS. 2(a)-2(f), ordinate 202 represents optical intensity of the pulses. Further, in FIGS. 2(a)-2(f) abscissa 204 represents time, in FIGS. 2(g)-2(h) abscissa 206 represents frequency of the pulses, and ordinate 208 represents amplitude of the pulses. In particular, FIG. 2(a) represents referenced pulses (IR) or pulses from the reference arm 112. At a given instant in time, a position of the reference device 110, such as a location of the time delay device along the direction 111, is selected such that one or more sample locations at a particular location (or depth) along the optical path length are selected. FIG. 2(b) represents pulses (Is) from the sample arm 114 that correspond to sample locations Xl, X2, X3, and X4 that are represented in FIG. 1 by reference numerals 130, 132, 134, and 136 respectively. In particular, pulses that are returned after interacting with the sample position X1 130 are represented by reference numerals 212, and pulses returned from the sample location X2 132 are represented by reference numerals 214. Similarly, pulses returned from the sample locations X3 134 and X4 136 are represented by reference numerals 216 and 218. It should be noted that the sample 108 may have fewer or more than 4 locations that need to be detected for distributed measurement.
Referring to FIGS. 2(a)-2(h), interference of pulses from a reference arm, for example, the reference arm 112 of FIG. 1 and a sample arm, for example, the sample arm 114 of FIG. 1 is illustrated. In FIGS. 2(a)-2(f), ordinate 202 represents optical intensity of the pulses. Further, in FIGS. 2(a)-2(f) abscissa 204 represents time, in FIGS. 2(g)-2(h) abscissa 206 represents frequency of the pulses, and ordinate 208 represents amplitude of the pulses. In particular, FIG. 2(a) represents referenced pulses (IR) or pulses from the reference arm 112. At a given instant in time, a position of the reference device 110, such as a location of the time delay device along the direction 111, is selected such that one or more sample locations at a particular location (or depth) along the optical path length are selected. FIG. 2(b) represents pulses (Is) from the sample arm 114 that correspond to sample locations Xl, X2, X3, and X4 that are represented in FIG. 1 by reference numerals 130, 132, 134, and 136 respectively. In particular, pulses that are returned after interacting with the sample position X1 130 are represented by reference numerals 212, and pulses returned from the sample location X2 132 are represented by reference numerals 214. Similarly, pulses returned from the sample locations X3 134 and X4 136 are represented by reference numerals 216 and 218. It should be noted that the sample 108 may have fewer or more than 4 locations that need to be detected for distributed measurement.
[0029] FIG.
2(c) represents the second plurality of pulses 210 that are from the second ultrafast laser source 104. FIG. 2(d) represents combined pulses from the reference device 110, the sample 108, and the pulses from the second ultrafast laser source 104 at the detector unit 124. In particular, FIG. 2(d) represents a summation of referenced pulses (IR) from the reference arm 112, the second plurality of pulses from the second ultrafast laser source 104, and processed or interacted pulses from the plurality of locations, such as locations X1 , X2, X3, X4 130-136 in the sample 108 are allowed to interfere. In one embodiment, the detector unit 124 is configured to perform nonlinear operations to provide an interferogram signal (ID), as represented in Equation (2) below:
= Equation (2) where ID represents interferogram signal, IR represents referenced pulses from the reference arm, Is represents pulses from the sample arm, and IL
represents the second plurality of pulses from the second ultrafast laser source 104.
2(c) represents the second plurality of pulses 210 that are from the second ultrafast laser source 104. FIG. 2(d) represents combined pulses from the reference device 110, the sample 108, and the pulses from the second ultrafast laser source 104 at the detector unit 124. In particular, FIG. 2(d) represents a summation of referenced pulses (IR) from the reference arm 112, the second plurality of pulses from the second ultrafast laser source 104, and processed or interacted pulses from the plurality of locations, such as locations X1 , X2, X3, X4 130-136 in the sample 108 are allowed to interfere. In one embodiment, the detector unit 124 is configured to perform nonlinear operations to provide an interferogram signal (ID), as represented in Equation (2) below:
= Equation (2) where ID represents interferogram signal, IR represents referenced pulses from the reference arm, Is represents pulses from the sample arm, and IL
represents the second plurality of pulses from the second ultrafast laser source 104.
[0030] The multiplication of pulses from different locations Xl, X2, X3, X4 130-136, and the pulses (IR) from the reference arm 112 causes the signals other than ones having same path length as that of the pulses from the reference arm to reduce to zero. Accordingly, as represented by FIG. 2(e), when the reference is moved such that the path length of the reference overlaps with signals from X1 130, the interferogram signal (ID) includes the interferogram of the signal from locationsX1 130 in the sample 108. Similarly generated interferogram signals for X2 132 are illustrated in FIG. 2(f). Further, interferogram signals from other locations, X3, and X4 134, and 136 may be obtained by correspondingly adjusting the reference device 110, for example by moving the reference mirror.
[0031] FIGS.
2(g)-2(h) illustrate Fourier transform of the interferogram signals corresponding to positions X1 130 and X2 132. Accordingly, the pulses represented by reference numerals 230 and 232 represent Fourier transforms of signals from positions X1 and X2 of the sample. The Fourier transforms, such as the Fourier transforms 230 and 232, are used to form an absorption profile of the sample 108 corresponding to corresponding sample locations as represented in FIG. 2(i). Equation (3) represents absorption profile at location X2 as:
C(z)-C(z-Az) A(z) = Equation (3) where, A(z) represents absolute absorption value at a location z in the sample, C(z) represents cumulative absorption value at the location z, and C(z-Az) represents cumulative absorption at a location z-Az, where the location z-Az is immediately before the location n in the path of the optical pulses. For example, if z represents location X2, z-Az may represent location X1 . The absorption profile as represented in FIG. 2(i) includes a peak 244 and has abscissa 240 that represents wavelength, and ordinate 242 that represents absorption values. In certain embodiments, height, width, and position of a peak, such as the peak 244 in the absorption profile may be used to measure various parameters, such as, but not limited to, temperature, pressure, concentration, composition, and the like.
In the illustrated example, a height 246 of the peak 244 is representative of the concentration of a particular species or concentration of the sample 108 in general.
Further, a width 248 and a position 250 of the peak 244 are representative of temperature and pressure, respectively, of the sample 108 at that particular location.
Distributed measurements can be carried out at several locations in the sample with a spatial resolution that is proportional to the pulse width of the ultrafast laser sources 102 and 104.
2(g)-2(h) illustrate Fourier transform of the interferogram signals corresponding to positions X1 130 and X2 132. Accordingly, the pulses represented by reference numerals 230 and 232 represent Fourier transforms of signals from positions X1 and X2 of the sample. The Fourier transforms, such as the Fourier transforms 230 and 232, are used to form an absorption profile of the sample 108 corresponding to corresponding sample locations as represented in FIG. 2(i). Equation (3) represents absorption profile at location X2 as:
C(z)-C(z-Az) A(z) = Equation (3) where, A(z) represents absolute absorption value at a location z in the sample, C(z) represents cumulative absorption value at the location z, and C(z-Az) represents cumulative absorption at a location z-Az, where the location z-Az is immediately before the location n in the path of the optical pulses. For example, if z represents location X2, z-Az may represent location X1 . The absorption profile as represented in FIG. 2(i) includes a peak 244 and has abscissa 240 that represents wavelength, and ordinate 242 that represents absorption values. In certain embodiments, height, width, and position of a peak, such as the peak 244 in the absorption profile may be used to measure various parameters, such as, but not limited to, temperature, pressure, concentration, composition, and the like.
In the illustrated example, a height 246 of the peak 244 is representative of the concentration of a particular species or concentration of the sample 108 in general.
Further, a width 248 and a position 250 of the peak 244 are representative of temperature and pressure, respectively, of the sample 108 at that particular location.
Distributed measurements can be carried out at several locations in the sample with a spatial resolution that is proportional to the pulse width of the ultrafast laser sources 102 and 104.
[0032] In some embodiments, the system 100 is configured for short distance measurements in a range from about 100 microns to few cms, and long distance measurements in a range from about few cms to few kms. Further, in some other embodiments, the system 100 is conductive for upto about c/fr of the laser, where c is the speed of light and fr is repetition rate of the ultrafast laser source. In certain other embodiments, the systems and methods of the present application may be configured for long distance distributed measurements, such as in oil and gas pipelines.
[0033] FIG. 3 illustrates another example of the system 300 for distributed measurements of a plurality of locations in a sample. Further, the system 300 is configured for long distance measurements, such as, but not limited to, down hole applications, spatial profiling of gas, oil, water in down hole systems, spatial gas concentration measurements in gas turbine exhaust, and health monitoring of coatings, such as, but not limited to, thermal barrier coatings on turbine blades. The system 300 includes first, second, and third ultrafast laser sources 302, 304, and 306 configured to provide first, second and third plurality of pulses. In a non-limiting example, the first, second, and third ultrafast laser sources 302, 304, and 306 are femtosecond laser sources. In some embodiments, the ultrafast laser sources 302, 304, and 306 may be in operative communication with other components of the system 300 via one or more optical fibers. In one embodiment, an optical fiber may be in operative communication with the first ultrafast laser source 302 such that at least a portion of the first plurality of pulses traverses through at least a portion of the optical fiber.
[0034] Further, the ultrafast laser sources 302 and 306 are operatively coupled to a reference clock 308 to synchronize the two sources 302 and 306 with respect to one another. Moreover, a reference device, such as a phase delay generator 310, is coupled to one of the first and third ultrafast laser sources 302 and 306.
In the presently contemplated example, where the phase delay generator 310 is coupled to the third ultrafast laser source 306, the phase delay introduced by the phase delay generator 310 to the third plurality of pulses of the third ultrafast laser source 306 in turn introduce a phase delay in the clock 308. Further, the phase delay introduced in the third plurality of pulses by the phase delay generator 310 results in a time delay being introduced in the third plurality of pulses with respect to the first plurality of pulses from the first ultrafast laser source 302. The third ultrafast laser source 306 along with the reference clock 308 acts as the reference arm to provide referenced pulses.
In the presently contemplated example, where the phase delay generator 310 is coupled to the third ultrafast laser source 306, the phase delay introduced by the phase delay generator 310 to the third plurality of pulses of the third ultrafast laser source 306 in turn introduce a phase delay in the clock 308. Further, the phase delay introduced in the third plurality of pulses by the phase delay generator 310 results in a time delay being introduced in the third plurality of pulses with respect to the first plurality of pulses from the first ultrafast laser source 302. The third ultrafast laser source 306 along with the reference clock 308 acts as the reference arm to provide referenced pulses.
[0035] In operation, the first plurality of pulses from the first ultrafast laser source 302 are passed through a circulator 312 and a portion 315 of the first plurality of pulses that are passed through the circulator 312 is used to interrogate the sample 314. A collimator 316 is used to collimate the pulses 315 passing through the circulator 312 towards the sample 314. Various sample locations in the direction 326 of the pulses from the collimator 316 are represented as X1 318, X2 320, X3 322, and X4 324. After interaction with the sample 314, the interacted pulses are combined with the third plurality of pulses using a combinator 328.
The combined pulses are then further combined with the second plurality of pulses from the second ultrafast laser source 304 using another combinator 330, to form resultant pulses. The repetition rates of the first and third ultrafast laser sources 302 and 306 are same. Further, the repetition rates of the first and third ultrafast laser sources 302 and 306 are relatively different from a repetition rate of the second source 304.
The combined pulses are then further combined with the second plurality of pulses from the second ultrafast laser source 304 using another combinator 330, to form resultant pulses. The repetition rates of the first and third ultrafast laser sources 302 and 306 are same. Further, the repetition rates of the first and third ultrafast laser sources 302 and 306 are relatively different from a repetition rate of the second source 304.
[0036] The resultant pulses are detected by a detector unit 332 and processed using a processor unit 334. Results, such as shown in FIG.s. 2(a)-2(i) may be displayed on a display device 336, such as a monitor, a touch screen, or the like.
[0037] FIG. 4 illustrates an example flow chart 400 for a method for distributed measurement at a plurality of locations in a sample to detect one or more parameters of the sample. At block 402, the method commences by providing a first plurality of pulses in a picosecond time domain or lower, and comb frequencies having a first repetition rate. At block 404, a portion of the first plurality of pulses is allowed to interact at the plurality of locations in the sample to provide processed pulses.
At block 406, a variable time delay, a variable phase delay, a variable path length difference, or combinations thereof, is introduced in another portion of the first plurality of pulses to provide referenced pulses. At block 408, a second plurality of pulses in a picosecond time domain or lower, and comb frequencies having a second repetition rate is provided. The second repetition rate is different from the first repetition rate.
At block 406, a variable time delay, a variable phase delay, a variable path length difference, or combinations thereof, is introduced in another portion of the first plurality of pulses to provide referenced pulses. At block 408, a second plurality of pulses in a picosecond time domain or lower, and comb frequencies having a second repetition rate is provided. The second repetition rate is different from the first repetition rate.
[0038] At block 410, at least a portion of the processed pulses from the first ultrafast laser source, the second plurality of pulses from the second ultrafast laser source, and the referenced pulses are detected by a detector. At bock 412, the detected pulses are processed to provide measurements of one or more parameters for the plurality of locations in the sample.
[0039] In some embodiments, a third plurality of pulses may also be provided.
In these embodiments, the time delay, phase delay, or path length difference may be introduced in one of the first or third plurality of pulses. Further, the first and third plurality of pulses may be synchronized. Moreover, the processed pulses may be combined with the third plurality of pulses.
In these embodiments, the time delay, phase delay, or path length difference may be introduced in one of the first or third plurality of pulses. Further, the first and third plurality of pulses may be synchronized. Moreover, the processed pulses may be combined with the third plurality of pulses.
[0040] The systems 100 and 300 of FIGS. 1 and 3 and methods of FIG. 2(a)-2(i) and FIG. 4 are configured for multispecies determination. By way of example, when interrogating a gaseous sample, different gases present in the gaseous sample may be detected using the systems and methods of the present application.
Advantageously, the systems and methods of the present application provide high resolution and faster measurement times. High resolution sensing allows identification of multiple materials simultaneously. Also, the systems and methods of the present application facilitate complete optical spectrum to determine multiple parameters instead of measuring these parameters individually. Moreover, the broadband and coherent output of the frequency combs also facilitates high signal-to-noise ratios. Also short pulse width of ultrafast lasers provide high spatial resolution.
Advantageously, the systems and methods of the present application provide high resolution and faster measurement times. High resolution sensing allows identification of multiple materials simultaneously. Also, the systems and methods of the present application facilitate complete optical spectrum to determine multiple parameters instead of measuring these parameters individually. Moreover, the broadband and coherent output of the frequency combs also facilitates high signal-to-noise ratios. Also short pulse width of ultrafast lasers provide high spatial resolution.
[0041] While only certain features of the invention have been illustrated and described herein, many modifications and changes will occur to those skilled in the art. It is, therefore, to be understood that the appended claims are intended to cover all such modifications and changes as fall within the scope of the invention.
Claims (17)
1. A system (100) for interrogating one or more parameters at a plurality of locations in a sample (108), comprising:
a first ultrafast laser source (102) configured to provide a first plurality of pulses in a picosecond time domain or lower, wherein the first ultrafast laser source (102) is configured to provide comb frequencies having a first repetition rate, and wherein the first plurality of pulses interacts with the sample (108) at the plurality of locations in the sample (108) to provide processed pulses;
a second ultrafast laser source (104) configured to provide a second plurality of pulses in a picosecond time domain or lower, wherein the second ultrafast laser source (104) is configured to provide comb frequencies having a second repetition rate that is different from the first repetition rate;
a reference device (110) configured to provide referenced pulses having a variable time delay, a variable phase delay, a variable path length difference, or combinations thereof;
a detector unit (124) configured to detect at least a portion of the processed pulses from the first ultrafast laser source (102), the second plurality of pulses from the second ultrafast laser source (104), and the referenced pulses; and a processor unit (128) configured to process the detected pulses and provide measurements of the one or more parameters for the plurality of locations in the sample (108).
a first ultrafast laser source (102) configured to provide a first plurality of pulses in a picosecond time domain or lower, wherein the first ultrafast laser source (102) is configured to provide comb frequencies having a first repetition rate, and wherein the first plurality of pulses interacts with the sample (108) at the plurality of locations in the sample (108) to provide processed pulses;
a second ultrafast laser source (104) configured to provide a second plurality of pulses in a picosecond time domain or lower, wherein the second ultrafast laser source (104) is configured to provide comb frequencies having a second repetition rate that is different from the first repetition rate;
a reference device (110) configured to provide referenced pulses having a variable time delay, a variable phase delay, a variable path length difference, or combinations thereof;
a detector unit (124) configured to detect at least a portion of the processed pulses from the first ultrafast laser source (102), the second plurality of pulses from the second ultrafast laser source (104), and the referenced pulses; and a processor unit (128) configured to process the detected pulses and provide measurements of the one or more parameters for the plurality of locations in the sample (108).
2. The system (100) of claim 1, wherein the first ultrafast laser source, the second ultrafast laser source, or both comprise a femtosecond laser source.
3. The system (100) of claim 1, wherein the reference device (110) comprises a time delay device, a phase difference generator, or a path length difference generator, or combinations thereof
4. The system (100) of claim 3, wherein the time delay device is a mirror.
5. The system (100) of claim 1, further comprising a third ultrafast laser source (306) configured to provide a third plurality of pulses.
6. The system (100) of claim 5, further comprising a clock (310) operatively coupled to the first and third ultrafast laser sources (302, 306) to synchronize the first and third ultrafast sources.
7. The system (100) of claim 6, further comprising a phase difference generator operatively coupled to the third ultrafast laser source (306).
8. The system (100) of claim 5, further comprising a circulator (312) operatively coupled to the first ultrafast laser source (102) to direct at least a portion of the interacted pulses such that the interacted pulses are combined with the third plurality of pulses.
9. The system (100) of claim 1, further comprising an optical fiber in operative communication with the first ultrafast laser source (102) such that at least a portion of the first plurality of pulses traverses through at least a portion of the optical fiber.
10. The system (100) of claim 1, further comprising an optical fiber in operative communication with the second ultrafast laser source (104) such that at least a portion of the second plurality of pulses traverses through at least a portion of the optical fiber.
11. The system (100) of claim 1, wherein the reference device (110) comprises a liquid crystal, a micro array, a micro electro mechanical system (MEMS), or an optical structure that is configured to introduce a time delay, a phase delay, or an optical path length difference.
12. A system (100) for interrogating one or more parameters at a plurality of locations in a sample (108), comprising:
a first femtosecond laser source (102) configured to provide a first plurality of pulses in a picosecond time domain or lower, wherein the first femtosecond laser source(102) is configured to provide comb frequencies having a first repetition rate;
and wherein the first plurality of pulses interacts with the sample (108) at the plurality of locations in the sample (108) to provide processed pulses;
a second femtosecond laser source (104) configured to provide a second plurality of pulses in a picosecond time domain or lower, wherein the second femtosecond laser source (104) is configured to provide comb frequencies having a second repetition rate that is different from the first repetition rate;
a reference device (110) configured to provide referenced pulses having a variable time delay, a variable phase delay, a variable path length difference, or combinations thereof;
a detector unit (124) configured to detect at least a portion of the processed pulses from the first femtosecond laser source (102), the second plurality of pulses from the second femtosecond laser source (104), and the referenced pulses; and a processor unit (128) configured to process the detected pulses and provide measurements of the one or more parameters for the plurality of locations in the sample.
a first femtosecond laser source (102) configured to provide a first plurality of pulses in a picosecond time domain or lower, wherein the first femtosecond laser source(102) is configured to provide comb frequencies having a first repetition rate;
and wherein the first plurality of pulses interacts with the sample (108) at the plurality of locations in the sample (108) to provide processed pulses;
a second femtosecond laser source (104) configured to provide a second plurality of pulses in a picosecond time domain or lower, wherein the second femtosecond laser source (104) is configured to provide comb frequencies having a second repetition rate that is different from the first repetition rate;
a reference device (110) configured to provide referenced pulses having a variable time delay, a variable phase delay, a variable path length difference, or combinations thereof;
a detector unit (124) configured to detect at least a portion of the processed pulses from the first femtosecond laser source (102), the second plurality of pulses from the second femtosecond laser source (104), and the referenced pulses; and a processor unit (128) configured to process the detected pulses and provide measurements of the one or more parameters for the plurality of locations in the sample.
13. The system (100) of claim 12, further comprising a third femtosecond laser source.
14. The system (100) of claim 12, wherein the reference device (110) is operatively coupled to the first femtosecond laser source.
15. The system (100) of claim 12, further comprising a collimator disposed between the first femtosecond laser source and at least a portion of the sample.
16. The system (100) of claim 12, further comprising an optical fiber in operative communication with the first femtosecond laser source such that at least a portion of the first plurality of pulses traverses through at least a portion of the optical fiber.
17. A method (400) for interrogating one or more parameters at a plurality of locations in a sample, comprising:
providing a first plurality of pulses in a picosecond time domain or lower, wherein the first plurality of pulses comprises a first repetition rate (402);
interacting a portion of the first plurality of pulses at the plurality of locations in a sample to provide processed pulses (404);
introducing a variable time delay, a variable phase delay, a variable path length difference, or combinations thereof in another portion of the first plurality of pulses to provide referenced pulses (406);
providing a second plurality of pulses in a picosecond time domain or lower, wherein the second plurality of pulses comprise a second repetition rate that is different from the first repetition rate (408);
detecting at least a portion of the processed pulses from the first ultrafast laser source, the second plurality of pulses from the second ultrafast laser source, and the referenced pulses (410); and processing the detected pulses to provide measurements of the one or more parameters for the plurality of locations in the sample (412).
providing a first plurality of pulses in a picosecond time domain or lower, wherein the first plurality of pulses comprises a first repetition rate (402);
interacting a portion of the first plurality of pulses at the plurality of locations in a sample to provide processed pulses (404);
introducing a variable time delay, a variable phase delay, a variable path length difference, or combinations thereof in another portion of the first plurality of pulses to provide referenced pulses (406);
providing a second plurality of pulses in a picosecond time domain or lower, wherein the second plurality of pulses comprise a second repetition rate that is different from the first repetition rate (408);
detecting at least a portion of the processed pulses from the first ultrafast laser source, the second plurality of pulses from the second ultrafast laser source, and the referenced pulses (410); and processing the detected pulses to provide measurements of the one or more parameters for the plurality of locations in the sample (412).
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| US5814820A (en) * | 1996-02-09 | 1998-09-29 | The Board Of Trustees Of The University Of Illinois | Pump probe cross correlation fluorescence frequency domain microscope and microscopy |
| US8633437B2 (en) * | 2005-02-14 | 2014-01-21 | Board Of Trustees Of Michigan State University | Ultra-fast laser system |
| RU2384835C1 (en) * | 2008-12-15 | 2010-03-20 | Институт физики полупроводников Сибирского отделения Российской академии наук | Ellipsometre |
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| US9341516B2 (en) * | 2013-08-30 | 2016-05-17 | Agilent Technologies, Inc. | System for performing optical spectroscopy including interferometer |
| CN104316186B (en) * | 2014-07-07 | 2016-08-24 | 华东师范大学 | A kind of spectral measurement method of optically-based frequency comb |
| CN104316180B (en) * | 2014-11-02 | 2016-06-01 | 华东师范大学 | Based on two optical frequency com optical imaging methods of continuous Frequency Stabilized Lasers |
| US20160153835A1 (en) * | 2014-12-02 | 2016-06-02 | Imra America, Inc. | Comb resolved fourier transform spectroscopy |
| CN105548036B (en) * | 2015-12-08 | 2018-04-06 | 上海理工大学 | A kind of adaptive double light comb spectroscopic systems |
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| WO2018005987A1 (en) | 2018-01-04 |
| WO2018005987A8 (en) | 2019-03-14 |
| CN109328300A (en) | 2019-02-12 |
| RU2729950C2 (en) | 2020-08-13 |
| RU2018145350A (en) | 2020-07-30 |
| RU2018145350A3 (en) | 2020-07-30 |
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