WO2016208013A1 - Système lidar et procédé de mesure - Google Patents

Système lidar et procédé de mesure Download PDF

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Publication number
WO2016208013A1
WO2016208013A1 PCT/JP2015/068257 JP2015068257W WO2016208013A1 WO 2016208013 A1 WO2016208013 A1 WO 2016208013A1 JP 2015068257 W JP2015068257 W JP 2015068257W WO 2016208013 A1 WO2016208013 A1 WO 2016208013A1
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Prior art keywords
light
interferometer
scattered light
laser light
optical path
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PCT/JP2015/068257
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English (en)
Japanese (ja)
Inventor
慶孝 神
伸夫 杉本
智明 西澤
パブロ リストリ
リディア オテロ
エドアルド ケール
Original Assignee
国立研究開発法人国立環境研究所
ナショナル サイエンティフィック アンド テクニカル リーサーチ カウンシル
ミニストリー オブ ディフェンス
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Application filed by 国立研究開発法人国立環境研究所, ナショナル サイエンティフィック アンド テクニカル リーサーチ カウンシル, ミニストリー オブ ディフェンス filed Critical 国立研究開発法人国立環境研究所
Priority to JP2017516007A priority Critical patent/JP6243088B2/ja
Priority to PCT/JP2015/068257 priority patent/WO2016208013A1/fr
Priority to ARP160101883A priority patent/AR105105A1/es
Publication of WO2016208013A1 publication Critical patent/WO2016208013A1/fr

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    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N15/00—Investigating characteristics of particles; Investigating permeability, pore-volume or surface-area of porous materials
    • G01N15/06—Investigating concentration of particle suspensions
    • 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
    • G01N21/41—Refractivity; Phase-affecting properties, e.g. optical path length
    • G01N21/45—Refractivity; Phase-affecting properties, e.g. optical path length using interferometric methods; using Schlieren methods
    • 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
    • G01N21/49—Scattering, i.e. diffuse reflection within a body or fluid
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S7/00—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
    • G01S7/48—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S17/00
    • G01S7/481—Constructional features, e.g. arrangements of optical elements
    • Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02A—TECHNOLOGIES FOR ADAPTATION TO CLIMATE CHANGE
    • Y02A90/00—Technologies having an indirect contribution to adaptation to climate change
    • Y02A90/10—Information and communication technologies [ICT] supporting adaptation to climate change, e.g. for weather forecasting or climate simulation

Definitions

  • the present invention relates to a rider system, and more particularly, to a rider system including a high-spectral decomposition rider and a measurement method using the rider system.
  • a lidar (LIDAR: Light Detection and Ranging) system is known as an aerosol observation device in the atmosphere.
  • the rider system is a radar system using laser light, and various configurations are known (for example, see Non-Patent Documents 1 and 2).
  • an interferometer corresponding to the wavelength of the laser beam output from the light source is placed to convert the Mie scattered light component from the total scattered light including the Mie scattered light component and the Rayleigh scattered light component.
  • a technique for extracting only the Rayleigh scattered light component by removing the light is being studied. Accordingly, it has been considered that it is ideal to set the laser light from the light source to a single longitudinal mode in order to suitably separate the Rayleigh scattered light component and achieve high measurement performance.
  • a single longitudinal mode laser light source is very expensive.
  • a device for fixing the wavelength of the single longitudinal mode laser beam is required, and the configuration of the device is complicated. It is possible to become.
  • the present invention has been made in view of the above, and relates to a rider system having a simple apparatus configuration and capable of realizing high measurement performance, and a measurement method using the rider system.
  • a rider system includes a laser light source that emits multi-longitudinal mode laser light into the atmosphere, a condensing unit that collects scattered light with respect to the laser light, and An interferometer that enters the light collected by the light condensing unit and selectively passes the incident light based on a transmission spectrum having a plurality of transmission peaks at the same interval as the mode interval of the laser beam; and the interference And a detection unit that detects light emitted from the meter, and an analysis unit that performs analysis on the light detected by the detection unit.
  • a measurement method is a measurement method using a lidar system, which collects scattered light from the atmosphere by emitting laser light in a multi-longitudinal mode from the laser light source to the atmosphere. And condensing the collected light, and selectively passing the collected light by an interferometer based on a transmission spectrum having a plurality of transmission peaks at the same interval as the mode interval of the laser beam, A step of detecting light emitted from the interferometer at a detection unit; and a step of performing analysis on the light detected by the detection unit at the analysis unit.
  • a reference light incident unit that makes a part of light emitted from the laser light source enter the interferometer as reference light.
  • the interferometer can be adjusted using the reference light incident on the interferometer from the reference light incident portion.
  • analysis using the detection result of the reference light can be performed, higher measurement performance can be realized.
  • the interferometer interferes with an optical branching unit that splits the incident light in two, an optical path difference forming unit that provides an optical path difference between the two branched light beams, and two branched lights that are provided with the optical path difference.
  • the optical path difference forming means can change the optical path difference provided between the two branched lights.
  • the optical path difference in the interferometer becomes variable.
  • the optical path difference can be adjusted according to the type of the laser light source, or the optical path difference can be finely adjusted for detailed analysis. Therefore, high measurement performance can be realized with a simpler apparatus configuration.
  • the detection unit may be configured to detect light emitted from the interferometer while changing an optical path difference in the interferometer.
  • the wavelength of the transmission peak of the transmission spectrum changes, so by detecting the scattered light while moving the transmission peak, the scattered light from the atmosphere can be detected.
  • Such a more detailed analysis can be performed.
  • a rider system having a simple device configuration and capable of realizing high measurement performance, and a measurement method using the rider system.
  • FIG. 1 is a schematic configuration diagram of a rider system according to an embodiment of the present invention.
  • FIG. 2A is a diagram illustrating an example of an optical signal including Mie scattered light and Rayleigh scattered light.
  • FIG. 2B is a diagram illustrating an example of an optical signal obtained by separating only Rayleigh scattered light.
  • FIG. 3A is a scattered light spectrum of the light collected by the light collecting unit 20.
  • FIG. 3B is a diagram illustrating an example of a transmission spectrum by the interferometer 30.
  • FIG. 1 is a schematic configuration diagram showing an apparatus configuration of a rider system according to an embodiment of the present invention.
  • the rider system 1 includes a laser light source 10 that emits laser light, a condensing unit 20 that condenses backscattered light from molecules in the atmosphere by irradiating the laser light, and a condensing unit 20.
  • Interferometer 30 that selectively equalizes only the light of a specific wavelength among the light collected at, detectors 41 and 42 (detectors) that detect the light interfered by interferometer 30, and detectors 41,
  • an analysis unit 50 that performs analysis based on the detection result of 42.
  • the lidar system 1 (LIDAR: Light Detection and Ranging) shown in FIG. 1 is a system mainly used for observation of aerosols (suspended particulate matter) in the atmosphere.
  • aerosols sustained particulate matter
  • FIG. 1 When laser light is irradiated into the atmosphere, several types of interaction occur between the laser light and the atmosphere.
  • pulse laser light is emitted into the atmosphere, and the backscattered light from the aerosol in the atmosphere and the molecules constituting the atmosphere are measured. Based on the time from laser light emission to light reception, the distance from the light source to the position where the scattered light is generated (the distance to the scatterer) can be obtained.
  • the laser light A scattering coefficient on the optical path can be calculated. Thereby, when the laser beam is irradiated toward the atmosphere (upward), a distribution of the scattering coefficient corresponding to the altitude can be obtained.
  • the types of scattering used for lidar measurement include Mie scattering by aerosol, Rayleigh scattering by atmospheric constituent molecules, and Raman scattering. Using these, the spatial distribution of aerosol, atmospheric density, concentration distribution of atmospheric components, etc. are measured. In addition, paying attention to the absorption received by the molecules in the atmosphere while the laser beam travels back and forth to the scatterer, the difference for obtaining the spatial distribution of the concentration of the absorbing molecules from the ratio of the two wavelength lidar signals of the large absorption wavelength and the small absorption wavelength There are methods such as absorption method.
  • the rider system 1 is a high spectral resolution lidar (High Spectral Resolution Lidar: HSRL) using Rayleigh scattering.
  • HSRL High Spectral Resolution Lidar
  • Conventionally used Mie scattering lidar is a system that receives and analyzes an optical signal including Mie scattered light derived from aerosol and Rayleigh scattered light derived from atmospheric constituent molecules.
  • the HSRL is a system capable of acquiring an optical signal including Mie scattered light and Rayleigh scattered light and an optical signal obtained by separating only the Rayleigh scattered light from the optical signal.
  • FIG. 2A is a diagram illustrating an example of an optical signal including Mie scattered light and Rayleigh scattered light.
  • FIG. 2B is a diagram illustrating an example of an optical signal obtained by separating only Rayleigh scattered light. 2A and 2B, the horizontal axis is the intensity of the optical signal, and the vertical axis is the altitude.
  • the intensity (signal intensity) of the scattered light generated at each altitude due to the irradiation of the laser light is attenuated toward the higher layer, but the intensity of the scattered light is larger in the aerosol layer.
  • the conventional Mie scattering lidar acquires only this information and analyzes the optical characteristics of the aerosol layer.
  • HSRL acquires an optical signal obtained by separating only Rayleigh scattered light.
  • a change in the intensity of scattered light derived from atmospheric constituent molecules can be acquired by the lidar system.
  • information on Rayleigh scattered light derived from atmospheric constituent molecules in the aerosol layer at altitudes h1 to h2 is acquired and combined with information obtained by mixing Mie scattered light and Rayleigh scattered light shown in FIG.
  • Information related to Mie scattered light can be extracted with higher accuracy.
  • the extinction coefficient ( ⁇ ) and the backscattering coefficient ( ⁇ ) which are information indicating the optical characteristics of the aerosol layer, can be extracted, and the aerosol layer can be analyzed with higher accuracy.
  • the rider system 1 can realize the above HSRL with a simpler device configuration.
  • the rider system 1 is characterized by a configuration in which the Mie scattered light component and the Rayleigh scattered light component are separately measured in the HSRL system. Therefore, in the following embodiments, a detection mechanism that separates and detects the Mie scattered light component and the Rayleigh scattered light component will be particularly described.
  • the laser light source 10 is a light source that emits laser light.
  • the laser light source 10 for example, an Nd: YAG laser can be used.
  • the second harmonic (wavelength 532 nm) of the Nd: YAG laser can be used as the laser light, but the wavelength of the laser light emitted from the laser light source 10 is not particularly limited.
  • an Nd: YLF laser can also be used.
  • laser light in a multi-longitudinal mode vertical multi-mode
  • the laser light source 10 can be prepared at low cost.
  • Laser light emitted from the laser light source 10 passes through the two mirrors 11 and the beam splitter 12 (reference light incident part), and the laser light reflected by the mirror 13 is emitted into the atmosphere.
  • the beam splitter 12 the laser light emitted from the laser light source 10 is input, the input light is branched into two, one branched light is emitted toward the mirror 13, and the other branched light is used as a reference light to collect the light.
  • the light is emitted toward 20.
  • the reference light is used for adjustment of the interferometer 30, and the details will be described later.
  • the condensing unit 20 has a function of condensing backscattered light generated by emitting laser light from the laser light source 10 into the atmosphere, and is realized by, for example, an astronomical telescope.
  • the light condensed by the condensing unit 20 is collimated by the collimating lens 22 through the field stop 21. Thereafter, the collimated light enters the interferometer 30 via the mirror 23.
  • a beam splitter is provided after the mirror 23, and a part of the light branched by the beam splitter is directly measured by the detector 43. It is good also as a structure.
  • the detector 43 is also connected to the analysis unit 50 described later, so that the result measured by the detector 43 can be used for analysis in the analysis unit 50.
  • the light transmittances detected by the two detectors 41 and 42 are opposite to each other as in the rider system 1 according to the present embodiment, they are detected by the two detectors 41 and 42. Since the total scattered light can be calculated based on the light information, the detector 43 need not be provided separately.
  • the interferometer 30 is a so-called Mach-Zehnder interferometer.
  • the collimated light incident through the mirror 23 is branched into two by a beam splitter 31 (light branching means), and one of the branched lights travels straight, while the other branched light. Is passed through a movable roof mirror 32 (optical path difference forming means).
  • the two branched lights have an optical path difference from each other.
  • These two branched lights are combined by a beam splitter 33 (light interference means) to interfere with each other.
  • the interval between the interference fringes formed by the interferometer 30 is set to correspond to the mode interval of the laser beam. This point will be described later.
  • the movable roof mirror 32 of the interferometer 30 can be realized, for example, by mounting a retro roof mirror on a piezo element. In this case, the optical path difference between the two branched lights can be adjusted by controlling the piezo element. However, if the movable roof mirror 32 can control the optical path difference between the two branched lights in the interferometer 30, the configuration thereof can be changed as appropriate.
  • the Mach-Zehnder interferometer 30 is used.
  • a Michelson interferometer, a Fabry-Perot interferometer, a Sagnac interferometer, a Fizeau interferometer, and the like have an interference having a periodic transmission spectrum.
  • a meter can also be used.
  • the detector 41 is arranged at a position where the light passing through the movable roof mirror 32 advances straight through the beam splitter 33.
  • the detector 42 is arranged at a position where the light that has traveled straight through the beam splitter 31 has traveled straight through the beam splitter 33. Thereby, the detectors 41 and 42 can detect signals whose phases are opposite to each other.
  • the analysis unit 50 acquires information on the Mie scattered light and the Rayleigh scattered light from the signals detected by the detectors 41 and 42 (and the detector 43 when the detector 43 is provided), It has a function of calculating an extinction coefficient ( ⁇ ) and a backscattering coefficient ( ⁇ ) indicating the optical characteristics of a certain aerosol layer.
  • the calculation method of the extinction coefficient ( ⁇ ) and the backscattering coefficient ( ⁇ ) in the analysis unit 50 does not depend on the type of the laser light source 10 or the like. Therefore, a known method can be used for calculating the extinction coefficient ( ⁇ ) and the backscattering coefficient ( ⁇ ). Specifically, for example, Zhaoyan Liu and two others, “High-spectral-resolution lidar using an iodine”, Optical Engineering, Vol. 38, No. 10, October 1999, p. Based on the method described in 1661-1670, the extinction coefficient ( ⁇ ) and the backscattering coefficient ( ⁇ ) indicating the optical characteristics of the aerosol can be calculated.
  • the rider system 1 is characterized in that a high-spectral resolution lidar (HSRL) system with high measurement accuracy is realized while using a laser beam in a multi-longitudinal mode. This point will be described with reference to FIG.
  • HSRL high-spectral resolution lidar
  • FIG. 3A is a scattered light spectrum of the light collected by the light collecting unit 20.
  • FIG. 3B is a diagram illustrating an example of a transmission spectrum by the interferometer 30.
  • scattered light including Mie scattered light and Rayleigh scattered light is acquired by the light collecting unit 20.
  • the Mie scattered light component S1 corresponds to the shape of the laser light emitted from the laser light source 10, as shown in FIG.
  • a peak P1 is formed for each mode interval with respect to the wavelength.
  • the Rayleigh scattered light component S2 has Doppler broadening, as shown in FIG.
  • the Rayleigh scattered light component S2 has a gentle peak P2 having broadening compared to the Mie scattered light component S1.
  • the peak P2 of the Rayleigh scattered light component S2 has a shape that fills the interval between laser light modes (between adjacent peaks P1). Therefore, the peak P1 of the adjacent Mie scattered light component S1 is between the peaks P1. If scattered light in the wavelength region is detected, information including the Rayleigh scattered light component S2 can be acquired.
  • the lidar system 1 is configured to control the interferometer 30 to remove the Mie scattered light component S1.
  • the interferometer 30 is a Mach-Zehnder type, the interval W2 of the interference fringes can be adjusted by adjusting the optical path difference of the two-branched light.
  • a transmission spectrum of such an interferometer 30 is shown in FIG. In the interferometer 30, light having a wavelength that forms a downward peak P ⁇ b> 3 of the transmission spectrum cannot be transmitted by the interferometer 30.
  • the transmission spectrum indicating the wavelength of light transmitted by the interferometer 30 is a spectrum having a plurality of transmission peaks formed at every predetermined interval W2.
  • scattered light from the atmosphere by emitting multi-longitudinal mode laser light from the laser light source 10 is condensed (condensing step) by the condensing unit 20, and the collected light is converted into the mode interval of the laser light.
  • the analysis unit 50 uses the optical information of the aerosol layer to be analyzed based on the above two pieces of information. An extinction coefficient ( ⁇ ) and a backscattering coefficient ( ⁇ ) are calculated (step of performing analysis). Thereby, measurement by the rider system is completed.
  • the acquisition of the Rayleigh scattered light component S2 will be further described.
  • the interference fringes caused by the mode interval W1 of the scattered light and the interferometer 30 It is possible to remove a plurality of peaks P1 of the Mie scattered light component S1 by matching the interval W2.
  • the optical path difference length of the two-branched light in the interferometer 30 may be made to coincide with the length of the resonator in the laser light source 10.
  • the Mie scattered light component S1 can be substantially measured by detecting the total scattered light and the scattered light from which the Mie scattered light component S1 has been removed (Rayleigh scattered light component S2). Thereby, the extinction coefficient ( ⁇ ) and the backscattering coefficient ( ⁇ ) can be calculated.
  • the conventional Mie scattering lidar used a multi-longitudinal mode laser light source, whereas the high spectral resolution lidar (HSRL) system is premised on using a single longitudinal mode laser light source as the laser light source. It was. As described above, since the Mie scattered light component and the Rayleigh scattered light component are mixed in the scattered light collected by the light collecting unit 20 by irradiating the laser beam, only the Rayleigh scattered light component is present. This is because it has been considered that the Mie scattered light component can be reliably removed by reducing the wavelength band of the Mie scattered light component to be removed.
  • HSRL high spectral resolution lidar
  • the single longitudinal mode laser light source must include an acousto-optic device, an AD converter capable of high-speed response (100 Msps or more), etc., in order to emit single longitudinal mode laser light. Therefore, there is a problem that the device configuration becomes complicated. Furthermore, the detector subsequent to the light collecting unit 20 also needs to be provided with a high-resolution spectroscopic element in order to accurately remove the Mie scattered light component. Further, it is necessary to adjust the transmission wavelength of the spectroscopic element in accordance with the emission wavelength of the laser light, but this adjustment is technically difficult. As described above, the HSRL system using a light source that emits a laser beam in a single longitudinal mode has a high load from the cost and technical aspects of the apparatus, and it was difficult to easily install it for applications such as continuous observation. .
  • the rider system 1 uses a multi-longitudinal mode laser light source 10 which is cheaper than a single longitudinal mode laser light source.
  • the mode interval of laser light emitted from the multi-longitudinal mode laser light source 10 is constant, an interferometer having a transmission peak for each wavelength interval corresponding to the Mach-Zehnder interferometer 30 mode interval is realized. Can do. Therefore, the interferometer 30 can remove the Mie scattered light component S1 having a peak for each mode interval of the laser light.
  • the rider system 1 can use a cheaper light source as compared with the conventional HSRL system.
  • the multi-longitudinal mode laser light source is more stable from the viewpoint of laser power than the single longitudinal mode laser light source.
  • a Fabry-Perot interferometer for example, an etalon interferometer
  • an interferometer that suitably removes light of the wavelength is used in consideration of the fact that Mie scattered light also has a single wavelength because laser light of a single longitudinal mode is used.
  • a Fabry-Perot interferometer there is a problem in terms of cost.
  • the rider system 1 can employ a cheaper Mach-Zehnder interferometer 30 to realize a configuration capable of removing Mie scattered light from the laser light in the multi-longitudinal mode. Therefore, it is possible to realize a simpler apparatus configuration not only for the laser light source 10 but also for the interferometer 30. As described above, the rider system 1 according to the present embodiment can realize high measurement performance such that the Rayleigh scattered light component S2 can be separated and measured with a simpler apparatus configuration.
  • a part of the laser light emitted from the laser light source 10 by the beam splitter 12 is taken as reference light.
  • the reference light is a multi-longitudinal mode laser light and has a peak in a wavelength region in which a Mie scattered light component will be included. Therefore, by adjusting the optical path difference of the interferometer 30 so that the peak component in the reference light can be removed, the interferometer is in a state where the Mie scattered light component S1 can be removed from the total scattered light from the atmosphere. 30 can be controlled, and higher measurement performance can be realized.
  • the interference effect (transmission effect) by the interferometer 30 related to the reference light is measured in advance by measuring only the reference light through the interferometer 30. be able to. Therefore, it becomes possible to detect the bias component due to the transmission wavelength setting deviation, and the data can be used for correction when separating and measuring the Rayleigh scattered light component S2 from the detection result of the total scattered light.
  • the interferometer 30 since the interferometer 30 includes the movable roof mirror 32, the optical path difference between the two optical paths can be easily changed.
  • the fact that the optical path difference can be easily changed allows the interval W2 between the peaks of the transmission spectrum by the interferometer 30 to be easily changed.
  • the interval W2 between the peaks of the transmission spectrum hardly changes, and the peak position moves. Therefore, for example, even if the position of the peak of the laser light emitted from the laser light source 10 is changed, if the detection is performed while sweeping the optical path difference by, for example, one wavelength of the laser light, Mie scattered light in the laser light.
  • the position of the peak derived from the component S1 can be detected.
  • the optical path difference of the interferometer 30 corresponding to the laser light can be easily adjusted. Further, even when measurement is performed using laser light from the same laser light source 10, it is possible to perform measurement while changing the degree of interference by the interferometer 30, and it is possible to perform analysis from various directions. . In this case, for example, analysis of the ratio of the Mie scattered light component S1 and the ratio of the Rayleigh scattered light component S2 included in the total scattered light can be evaluated. Specifically, in a state where the mode interval of the laser beam is fixed, detection is performed while changing the optical path difference of the interferometer 30 by one wavelength of the laser beam, so that the Rayleigh scattered light component caused by the spectrum of the laser beam The bias component included in S2 can be evaluated.
  • the rider system 1 has a configuration that allows the two detectors 41 and 42 to individually detect signals having phases opposite to each other. Therefore, since the information regarding the transmission spectrum by the interferometer 30 can be acquired, the measurement sensitivity by the detectors 41 and 42 can be improved. In particular, when the detectors 41 and 42 are configured to detect signals having opposite phases, the obtained information can be applied to the control of the interferometer 30. Specifically, for example, a feedback system that performs control so as to optimize the optical path difference of the interferometer 30 based on signals detected by the detectors 41 and 42 can be constructed with higher accuracy.
  • the rider system and the measurement method by the rider system according to the embodiment of the present invention have been described.
  • the above-described embodiment shows an example of the present invention.
  • the rider system and the measurement method according to the present invention are not limited to the above-described embodiments, and may be modified within a range not changing the gist described in each claim, or applied to another.
  • the arrangement of optical elements and the like included in the rider system 1 of the above embodiment can be changed as appropriate.
  • the said embodiment demonstrated the case where the two detectors 41 and 42 were installed, there should just be at least one detector as a detection part.
  • the reference light is used for the adjustment of the interferometer 30, etc.
  • the structure which is not provided with the means to make the condensing part 20 condense may be sufficient. Even in that case, high measurement performance in the rider system 1 can be realized.
  • the reference light instead of the configuration in which the reference light is incident on the interferometer 30 via the light collecting unit 20, the reference light may be directly introduced into the interferometer 30. That is, the optical path for introducing the reference light into the interferometer 30 can be provided separately from the optical path for introducing the scattered light into the interferometer 30.
  • the order of measurement of the total scattered light and measurement of the Rayleigh scattered light component S2 may be changed.
  • the total scattered light may be measured by measuring the light collected by the light collecting unit 20 without using the interferometer 30. Therefore, the configuration for measuring the total scattered light can be added to the rider system 1 as appropriate, for example, like the detector 43.

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Abstract

La présente invention concerne un système lidar (1) qui utilise une source de lumière laser à multiples modes longitudinaux (10) qui est moins coûteuse qu'une source de lumière laser à un seul mode longitudinal. Le mode d'espacement de la lumière laser émise depuis une source de lumière laser à multiples modes longitudinaux (10) est également constant et il est, par conséquent, possible de réaliser un interféromètre ayant un pic de transmission pour chaque espacement de longueur d'onde correspondant au mode d'espacement, par le biais de l'utilisation d'un interféromètre de Mach-Zehnder (30). Par conséquent, une composante de lumière de diffusion de Mie (S1) ayant un pic pour chaque mode d'espacement de la lumière laser peut être retirée par l'interféromètre (30).
PCT/JP2015/068257 2015-06-24 2015-06-24 Système lidar et procédé de mesure WO2016208013A1 (fr)

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JP2017516007A JP6243088B2 (ja) 2015-06-24 2015-06-24 ライダーシステム及び計測方法
PCT/JP2015/068257 WO2016208013A1 (fr) 2015-06-24 2015-06-24 Système lidar et procédé de mesure
ARP160101883A AR105105A1 (es) 2015-06-24 2016-06-23 Lidiar de alta resolución espectral multimodo

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Cited By (9)

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