Patent Grant
10126163
This application is a National Stage of International patent application PCT/EP2016/050304, filed on Jan. 8, 2016, which claims priority to foreign French patent application No. FR 1500033, filed on Jan. 9, 2015, the disclosures of which are incorporated by reference in their entirety.
The field of the invention is that of fiber optic sensors. More precisely, it relates to sensors able to detect an excitation in proximity to the fiber, and also able to locate this excitation along the fiber in a noisy environment.
This type of sensor has many applications as a pressure sensor in particular, allowing, by detection of modulation of the phase of an optical wave, environmental variations to be detected. One of the fields of application in which this type of detection is particularly of interest is underwater detection.
The underwater detection of soundwaves is of fundamental importance for coastal surveillance and certain military applications (for example detection/identification of submarines and surface vessels, the detection of divers or drones, etc.) and for civil applications (bioacoustic applications, monitoring of underwater seismic activity, detection of noise in the environment, etc.). To this end, fiber optic sensors are widely used both for their sensitivity and their compactness. The most sensitive are based on active (laser) or passive Bragg gratings, coupled to a mechanical transducer that converts the radial pressure of the acoustic wave into elongation of the fiber leading to a change in phase or optical wavelength. Distributed feedback fiber laser (DFB-FL) sensors are capable of detecting picostrains i.e. relative variations of −ΔL/L˜10−12, as described in the article “All-optical acoustic array for underwater surveillance”, R. Bouffaron et al., PROCEEDINGS OF SPIE, volume 8794, paper 8794-36, Fifth European Workshop on Optical Fibre Sensors, Krakow 2013.
However, sensors and systems based on Bragg gratings are intrinsically sensitive to variations in the environment (typically temperature and static pressure variations), this placing large constraints on the design of this type of sensor and/or system.
Furthermore, to detect the associated optical phase modulation, precise interferometric measurements must be carried out, which are often a limitation on practical implementation of such systems, in particular when the detection must be executed in a fluctuating environment. Specifically, in this case, servocontrol mechanisms that are often onerous must be implemented in conventional interferometers to maintain quadrature, i.e. the optimal detection condition that allows the sensitivity of the sensor to be maximized.
To meet the needs of this type of application, requiring extreme sensitivities to the quantity to be measured and a relative insensitivity to environmental interference impacting the reading system, the Applicants have proposed in patent application FR 1302640 to use the high phase-change sensitivity delivered by the adaptive holography obtained by mixing two waves in a liquid-crystal light valve (LCLV), this type of valve being known in the prior art for its capacity to produce holograms by converting the intensity variation of an interference pattern into a variation in the index of the liquid crystal, thus inducing an optical phase variation. Typically, the LCLV comprises a thin layer of liquid crystal LC, typically of a thickness comprised between 10 and 200 μm, this layer being placed between two substrates, one of the substrates comprising a photoconductor PC able to convert the light received at N emission wavelengths λi into charge. For example, the layer of liquid crystals is located between a glass substrate and a substrate made of a photoconductor crystal, for example a crystal of BSO, that is sensitive to blue/green wavelengths, electrodes being deposited on the substrates.
Apart from its sensitivity, the passband of this detecting device allows slow fluctuations to be filtered and a sensor that is insensitive to variations in environmental conditions to be produced. In addition, this detecting device is coupled to a multimode fiber optic sensor, which is more sensitive to elongation than a single-mode fiber, and which therefore allows the sensing portion to be simplified and the transducer to even be made redundant.
Nevertheless, this solution has a drawback insofar as the heart of the interferometer is a liquid-crystal light valve that prevents independent optimization of the writing and reading of the hologram (the latter for example being adapted to the working wavelength) and insertion of a step of processing the signal in the interferometer.
To mitigate the aforementioned drawbacks, the Applicants propose a new fiber optic sensor using digital holography, replacing and thus disassociating the liquid-crystal valve with a video camera and a liquid-crystal spatial light modulator.
More precisely, one subject of the present invention is a fiber optic sensor for detecting an excitation in proximity to a fiber optic assembly, said excitation inducing a modulation of the phase of an optical signal propagating in said fiber optic assembly, said sensor comprising:
a laser assembly of at least one laser, said laser assembly being configured to emit at least one laser beam;
a fiber optic assembly having a first end and a second end;
an optical system configured to:
a digital holography assembly comprising:
at least one optical detector configured to detect an output optical signal beam resulting from:
a processing unit, connected to the output of said optical detector, for processing said output optical signal beam, allowing information relative to said excitation to be extracted.
According to one variant of the invention, the fiber assembly is multimode, allowing the sensitivity to strain to be increased.
According to variants of the invention, the fiber optic sensor comprises first means, possibly a first acousto-optical modulator, for generating optical pulses from said laser.
According to the present invention, use of an adaptive interferometer allows both a complex wavefront issued from the fiber optic assembly to be demodulated and low-frequency environmental interference to be filtered. The use of a video camera allows the interference pattern to be detected, and the liquid-crystal spatial light modulator allows the phase to be read.
According to one variant of the invention, provision is made for a beam splitter to split the signal beam and the reference beam into two portions, a first portion of said beams being directed to said video camera, the second portion of said beams being directed to the liquid-crystal spatial light modulator.
The fiber optic sensor may advantageously include a processing unit, for processing on output from said video camera said interference pattern and for addressing it to said liquid-crystal spatial light modulator. The processing carried out may typically be spatial and/or temporal filtering. Specifically, according to the invention, digital coding of the phase allows both the reading and writing of the phase grating to be independently optimized and a step of processing the signal to be inserted.
According to variants of the invention, the signal beam received by said first end is issued from a beam inserted at said second end and propagated in transmission in said fiber optic assembly.
According to variants of the invention, the signal beam received by said first end is issued from a beam inserted at said first end and backscattered in said fiber optic assembly.
According to variants of the invention, the liquid-crystal spatial light modulator operates in reflection.
Another subject of the invention is a fiber optic sensor operating in backscatter and advantageously including means allowing said excitation to be located.
According to variants, a first portion of the laser beam is temporally modulated before being inserted into the fiber optic assembly, a second portion of the laser beam forming the reference laser beam without being temporally modulated, the sequential arrival of the pulses allowing the location of said excitation level with the fiber optic assembly. Since the speed v of propagation of the light wave in the optical fiber is known, measuring the duration dt of a round trip of a pulse makes it possible to determine at what distance Li into the fiber, referenced from the end Ei, the latter was backscattered: 2×Li=v×dt.
According to variants of the invention, the reference beam is generated from said signal beam output from said first end and comprises means for creating a path difference in said reference beam.
According to variants of the invention, the fiber optic sensor comprises at least:
a circulator positioned:
a coupler located at the output of said fiber optic assembly for creating two optical channels carrying output optical pulses;
means for delaying said output pulses of said fiber optic assembly in one of said two channels so as to create a signal channel carrying signal optical pulses and a reference channel carrying reference optical pulses in order to generate said interference zones on said spatial light modulator.
According to variants of the invention, the sensor furthermore includes:
second means, possibly a second acousto-optical modulator located at the output of the circulator and at the input of the coupler allowing windows of duration 2ΔL/c, where c is the speed of light in free space and ΔL/2 is the length of a sensing zone defined between a position Ai and a position Bi in said fiber optic assembly and referenced from said first end, to be selected in order to let interfere only backscattered waves originating from a sensing zone of said fiber at the same time;
means for delaying said output pulses introducing an additional length to be traced ΔL;
the pulses being separated by a duration tR, such that tR>2L/c, the duration of said pulses tp being tp>ΔL/c and tR>toff where toff is the response time of the liquid crystals.
According to variants of the invention, the sensor furthermore comprises:
what is called a writing laser assembly comprising at least one laser emitting a series of what are called writing pulses at a pump frequency ωp and a laser beam emitting a series of what are called writing pulses at a signal frequency ωs that is different from the frequency ωp;
the optical system being configured:
According to variants of the invention, the writing laser assembly comprises:
said laser emitting a laser beam;
means for dividing said beam into two channels;
means for shifting the pump frequency ωp to a signal frequency ωs in one of the channels;
means for generating pulses in the two frequency-shifted optical channels, possibly acousto-optical modulators.
According to variants of the invention, said optical system is configured so that said reference beam or said reference pulses interfere, on being input into said liquid-crystal modulator without having been injected into said fiber optic assembly, with said signal optical pulses (IpsiS) issued from said optical pulses injected into then propagated in said fiber.
According to variants of the invention, said optical system is configured so that said reference beam or said reference pulses interfere, on being input into said liquid-crystal modulator after having been injected into said fiber optic assembly, with said signal optical pulses issued from said optical pulses injected into then propagated in said fiber.
According to variants of the invention, the fiber optic sensor for locating an excitation in proximity to a fiber optic assembly operates in reflection and comprises:
a laser assembly configured to emit N laser beams Fi indexed i with i>1 of respective wavelength λi;
a fiber optic assembly including N successive segments indexed i, each segment comprising a device Mi for selectively reflecting an associated emission wavelength λi, the indices being referenced with respect to one end of said fiber optic assembly;
the optical system generating N reference beams Fri indexed i of emission wavelength λi from a laser beam Fi and producing N interference zones indexed i, each zone corresponding to the interference between a reference beam Fri and a signal beam Fsi of same emission wavelength λi;
at least one optical detector configured to detect N output optical signals Fouti indexed i and respectively diffracted by said N holograms;
a processing unit suitable for identifying the segment of said fiber optic assembly located in proximity to said excitation to be located, from the N detected output optical signals Fouti.
According to variants of the invention, the fiber optic sensor for locating an excitation in proximity to a fiber optic assembly includes:
a laser assembly emitting a continuous-wave laser beam at a frequency f;
means for performing a periodic frequency scan of said frequency f in a frequency band [0, fm] so as to code backscattering planes Pi corresponding to lengths Li referenced with respect to one end of said fiber optic assembly;
means for obtaining a shift Δf in the frequency of the reference laser beam so as to inscribe a hologram in said liquid-crystal spatial light modulator when the frequency of the reference beam coincides with the frequency of the signal laser beam;
a processing unit suitable for identifying the position of a backscattering plane Pi referenced with respect to one end of said fiber optic assembly.
The invention will be better understood and other advantages will become apparent on reading the following nonlimiting description, and by virtue of the appended figures, in which:
The fiber optic sensor of the present invention is able to locate an excitation in proximity to a fiber optic assembly. The excitation that the sensor detects is such that it induces a modulation of the phase amplitude Δϕ of an optical signal propagating in the fiber optic assembly. The excitation for example corresponds to a pressure variation, in air (microphone type sensor) or in water (hydrophone type sensor) typically at a frequency higher than a few Hz and will be referenced A in the rest of the present description.
Generally, the fiber optic sensor of the present invention uses digital holography.
Digital holography is in particular described in the article by J. W. Goodman and R. W. Laurence, “Digital image formation from electronically detected holograms”, Appl Phys Lett 11, 77 (1967) and is a technology that is currently being developed in industry and scientific instrumentation, and that has various applications in metrology, nondestructive testing and probing techniques, microscopy and 3-D imaging as described in the article by U. Shnars and W. Juptner, Digital holography (Springer Ed. 2005). Even with very small signal intensities, photonic noise limited image reconstruction has been demonstrated, as described in the article by M. Gross and M. Atlan, “Digital holography at shot noise level”, Opt Lett. 32, 909 (2007). These recent developments are related to the availability on the market of video cameras that provide high resolutions, both in the visible and in the near-infrared, and of CCD and CMOS matrix array detectors with pixel sizes of the order of one micron. Another important aspect is the very high computational power currently available, allowing large images to be produced and quite complex interferograms to be reconstructed.
A new digital holography approach was introduced very recently for real-time phase conjugation of a segmented wavefront and for the demonstration of the coherent combination of fiber lasers as described in the article by C. Bellanger, A. Brignon, J. Colineau and J. P. Huignard, “Coherent fiber combining by digital holography”, Opt Lett. 33, 2937 (2008). In this approach, the digital holography system consists of a CCD detecting matrix array that controls a liquid-crystal (LC) spatial light modulator (SLM).
Apart from the coherent combination of fiber lasers, this configuration has also been used to demonstrate phase conjugation in a multimode fiber, in highly scattering media and for focusing and scanning through a multimode fiber with the aim of correcting phase shifts undergone by an optical fiber as described in the articles by M. Paurisse, M. Hanna, F. Druon, P. Georges, C. Bellanger, A. Brignon and J. P. Huignard, “Phase and amplitude control of a multimode LMA fiber beam by use of digital holography”, Opt Express 17, 13000 (2009), or by M. Cui and C. Yang, “Implementation of a digital optical phase conjugation system and its application to study the robustness of turbidity suppression by phase conjugation”, Opt Express, 18, 3444 (2010) or by I. Papadopoulos, S. Farahi, D. Psaltis, and C. Moser, “Focussing and scanning light through a multimode optical fiber using digital phase conjugation”, Opt Express. 20, 10583 (2012) or by I. Papadopoulos, O. Simandoux, S. Farahi, J. P. Huignard, E. Bossy, D. Psaltis and C. Moser, “Optical resolution photoacoustic microscopy by use of multimode fiber”, Appl Phys Lett, 102, 211106 (2013) or indeed by I. Papadopoulos, S. Farahi, D. Psaltis and C. Moser, “High resolution lensless endoscope based on digital scanning through a multimode optical fiber”, Biomed Opt Express 4, 260 (2013).
Nevertheless, these articles do not relate, as in the present invention, to the detection of an excitation by a fiber optic sensor capable of detecting very small perturbations.
The sensor of the invention comprises the combination of a fiber optic assembly possibly including a fiber that may advantageously be multimode as strain sensor and an adaptive interferometer based on digital holography, to detect a perturbation.
The two basic main components are thus a video camera CA, possibly a CCD or CMOS video camera and a liquid-crystal spatial light modulator SLM and these components are placed symmetrically at 45° about a 50% beam splitter Ls, and precisely imaged one on the other.
Thus, the coherent optical waves, i.e. the reference and the signal bearing the speckle pattern to be demodulated (optical phase modulation at the frequency Ω), are split by the beam splitter and superposed in order to interfere on the video camera CA.
The interference pattern obtained on the video camera is addressed electrically via a processing unit UNCA to the liquid-crystal spatial light modulator SLM (denoted LC SLM in the description below) in order to create the phase hologram that corresponds thereto.
This hologram allows the reference laser beam and the signal beam, which are incident directly on the LC SLM, to be diffracted. The signal diffracted in one of the diffraction orders is collected with a photodiode PD. Its frequency is that of the phase modulation in the fiber optic assembly. The amplitude of its intensity modulation is proportional to the amplitude of the phase modulation of the signal wave carried by the signal beam.
The reference and signal beams FrM and FsM are used to read the hologram thus inscribed. The I−1 diffraction order of the reference beam FdrM diffracted by the inscribed hologram and superposed on the 0 order of the transmitted laser beam of the signal FtSM may in particular be analyzed.
In the operating mode in
Mixing and interaction of optical waves in a multimode system has been described in the article by U. Bortolozzo, S. Residori and J. P. Huignard, “Beam-Coupling in Photorefractive Liquid Crystal Light-Valves”, J. Phys. D: Appl. Phys. 41, 224007 (2008), in the context of light valves and also allows in the context of the present invention very small phase perturbations to be effectively measured.
The liquid-crystal spatial light modulator may either operate in transmission, or in reflection as shown in
case (a): the video camera is turned off, the signal beam and the reference beam are transmitted;
case (b): the signal and reference laser beams are diffracted, the video camera is in operation allowing a diffraction hologram to be inscribed:
The total incident intensity is 0.4 mW/cm2.
a solid-state laser source used at a wavelength 532 nm;
a 5 m multimode fiber (numerical aperture NA=0.2 and a core diameter of d=200 microns);
a phase perturbation at the frequency 10 kHz with an amplitude of about 0.3 mrad induced in said optical fiber by a piezoelectric crystal;
digital holography achieved with a CMOS video camera (Photonfocus A1312, 1312×1080 pixels, pixel size of 8 microns, 8 bit) and a liquid-crystal spatial modulator (HOLOEYE, PLUTO operating in reflection as shown in
the image detected by the video camera is recorded by a computer and sent to the liquid-crystal spatial modulator;
detection of the modulation in the −1 order with a silicon photodiode.
The fiber optic sensor of the invention may also operate according to the principal described above and in a Rayleigh backscatter mode, as schematically shown in
The laser assembly SL forms a source that is split via a two-channel coupler, one channel being dedicated to the reference wave carried by the reference beam and one channel being dedicated to the signal wave carried by the beam Fs output from the fiber optic assembly, after insertion at the end E1 and propagation in the fiber optic assembly OF.
The sensor of the present invention may advantageously comprise means allowing the excitation to be located with respect to the extent of the fiber optic assembly defined between the two ends E1 and E2 when it functions in backscatter.
According to a first operating mode, shown in
2×Li=v×dt.
According to another operating mode, shown in
A path difference of length L generated by means Dm is thus added between the two (signal and reference) channels. These means may typically consist of a segment of optical fiber.
The two channels are transmitted to the interferometer. The interference between the pulse and its delayed replica allows the phase shift undergone by the fiber over a distance corresponding to L/2 to be measured. The sequential arrival of the pulses allows the perturbation to be located.
According to another operating mode, the fiber optic sensor may be exploited in a reflection mode, the fiber optic assembly OF being configured to integrate various wavelength-selective mirrors distributed along the fiber optic assembly.
The laser source assembly SL for its part forms a continuous-wave multi-wavelength source (possibly composed of a plurality of single-mode sources) emitting at wavelengths λ1, . . . , λi, . . . , λN. The multi-wavelength λi source is split into two channels: a reference channel including waves carried by the beams Fri, said waves being directed directly to the interferometer, and a channel intended for the waves carried by the signal beams Fsi output from the (single-mode or multimode) fiber optic assembly.
This fiber optic assembly is composed of N successive segments Ti indexed i, each segment comprising a selective reflecting device Mi able to reflect one associated emission wavelength λi, i.e. the reflection of which is centered on the wavelength λi. The reflecting devices are typically spaced apart by a distance d. Each segment of length d corresponds to a sensing portion of the sensor.
The indices i are referenced with respect to one end E1 of the fiber assembly OF, which end is located on the side of the laser assembly: the segment T1 reflecting the wavelength λ1 corresponds to the first segment, i.e. the segment closest to the end E1, and the segment TN reflecting the wavelength λN corresponds to the last segment, i.e. the segment furthest from the end E1.
According to one embodiment, each reflecting device Mi comprises a dichroic mirror. Preferably, in this case, the fiber optic assembly comprises N optical fibers OF1, . . . , OFi, . . . , OFN, each fiber OFi and the associated dichroic mirror MDi corresponding to one segment Ti.
According to another embodiment, each reflecting device Mi comprises a Bragg reflector. Preferably, in this case, the fiber optic assembly OF is formed from a single fiber OF0, the Bragg reflectors being integrated into the fiber OF0 using recording means that are known in the prior art.
The sensor according to the invention furthermore comprises an optical system configured to provide an array of optical functions.
First of all, the optical system is configured to inject, via the end E1 of the fiber optic assembly OF, the laser beams Fi emitted by the laser assembly SL, which will then propagate in the fiber. The beam F1 of wavelength λ1 passes through the first segment T1 and is reflected from the reflecting device M1. The other beams F2, . . . , Fi, Fi+1, . . . , FN of wavelength λ2, . . . , λi, λi+1, . . . , λN pass through the second segment T2. The segment Ti+1 is located between the mirror Mi and the mirror Mi+1. The beam of wavelength λ2 is reflected from the reflecting device M2 and so on until the last beam of wavelength λN, which alone passes through the last segment TN and is reflected from the reflecting device MN.
Thus, the fiber optic assembly receives, output from the end E1, N signal beams Fsi indexed i of wavelength λi output from the fiber optic assembly OF. Each signal beam Fsi is issued from the reflection from the reflecting means Mi, associated with the wavelength λi, of the laser beam Fi of wavelength λi injected into then propagated in the various segments of the fiber optic assembly OF, as described above.
The optical system is also configured to generate N reference beams Fri indexed i of wavelengths λi, from the laser beam Fi of emission wavelength λi.
With the reference beams Fri and the signal beams Fsi, the optical system is configured to produce N interference zones Zi indexed i, each zone corresponding to the interference between one reference beam Fri and one signal beam Fsi of same emission wavelength λi. Thus an interference zone Zi corresponds to the interference between the reference beam Fri issued directly from the laser on the one hand, and the signal beam Fsi injected into and propagated in the fiber optic assembly on the other hand, both of wavelength λi. The interference of Fri and Fsi gives rise to a pattern of intensity fringes.
The N interference zones are separate, or adjacent, or partially overlap, or are located in the same spatial location.
The optical detector PD, typically a photodiode, is configured to detect the N output optical signals Fouti indexed i diffracted by the N holograms Hi, respectively. The holograms Hi typically operate in a Raman-Nath diffraction regime, and various diffracted beams may be detected.
According to one embodiment, the optical detector is placed so as to detect, for each wavelength, the diffracted beam issued from the signal beam Fsi (in the same direction).
According to another embodiment, the optical detector is placed so as to detect, for each wavelength, the diffracted beam issued from the reference beam Fri (in the same direction).
According to another embodiment, the optical detector is placed so as to detect, for each wavelength, a diffracted beam of higher order.
The sensor includes a processing unit UNPD suitable for identifying the segment of the fiber assembly OF located in proximity to the excitation to be located. This identification is made on the basis of the N detected output optical signals. Specifically, each detected optical signal Fouti carries information on the phase modulation Δϕ, which may result in temporal modulation of its intensity about a frequency equal to the central frequency of the phase modulation Δϕ.
This information is detected by the detector PD, then processed by the processing unit UNPD in order to identify the segment closest to the external excitation that induced the phase modulation in the fiber.
According to one embodiment, the processing consists in determining, among the N detected output optical signals (Fouti), the output optical signal of lowest index k1 containing the phase modulation (i.e. an associated intensity modulation), the segment Tk1 to be identified corresponding to the segment having the index k1.
Specifically, if the excitation occurs in proximity to the segment T1 closest to the end E1, all the optical signals Fouti for all the wavelengths λi propagate through this segment, and are therefore modulated. The segment of lowest index is the segment T1.
More generally, if the excitation occurs in proximity to the segment Tk1 of index k1, only optical beams of indices higher than or equal to k1 propagate through the segment Tk1, optical beams of lower index 1, . . . , k1−1 having already been reflected from the corresponding reflecting devices M1, . . . , Mk1. Thus, the segment Tk1 is identified. Thus, the fiber optic assembly OF structured into segments forms a distributed sensor, wavelength multiplexing allowing the segment located in proximity to the external excitation to be identified.
According to another variant of the invention, the excitation is located by virtue of the use of a laser assembly SL forming a continuous-wave source that is frequency scanned periodically by means Bf that are for example able to perform direct modulation of the current of a laser diode or by an acousto-optical frequency translator, as schematically shown in
The source is split into two channels: a reference channel corresponding to a wave carried by the reference beam Fr, which is in addition frequency shifted by Δf by means Df, for example by an acousto-optical frequency translator or an electro-optical modulator, and directed toward the interferometer, and a channel issued from the laser beam inserted into the fiber optic assembly, and corresponding to a signal wave output from the (single-mode or multimode) fiber optic assembly.
Δf=2Lifm/(ctm)
The backscattered wave carried by the signal beam Fs contains the phase modulation to be detected and interferes with the reference in the interferometer.
The frequency shift Δf allows a hologram to be inscribed when the frequency of the reference arm coincides with the backscattered frequency, and therefore solely for one given backscattering plane. Location is therefore possible via variation of the value Δf. Δf is varied as a function of time in the form Δf=a×t (a being the rate of variation in frequency). The value of Δf that allows the “delay” seen by the wave injected into and then backscattered in the fiber therefore allows the inscription of a fixed pattern with the two waves and their diffraction in the liquid-crystal spatial modulator SLM. This known value of Δf allows the distance Li at which the wave was backscattered to be determined:
Δf=a×2×Li/v.
Generally, the sensor according to the invention has many advantages. It is low-cost, stealthy and easily deployable.
Another advantage of the present invention is that the sensor has a very high sensitivity. Specifically one important feature of adaptive holography is that, for small modulations of phase amplitude Δϕ, the detection is always linear in Δϕ and therefore the power measured in each output order is directly proportional to the amplitude of the phase modulation, and a direct measurement of Δϕ may be achieved by placing a photodiode on one of the diffracted orders at the output of the liquid-crystal spatial light modulator.
Because of the linear character of the detection, small signals, which otherwise would be hidden by noise, may be measured (for example, if the detection is quadratic the slope of the measurement curve, which gives sensitivity, is substantially smaller). In addition, sensitivity is also increased because of the large phase shift produced by the liquid-crystal spatial light modulator as a function of the variations in intensity.
This example relates to the production of a distributed fiber optic sensor allowing a perturbation to be located:
According to the exemplary configuration illustrated in
Thus, a pulse inserted into the optical fiber OF of length L, via a circulator C, gives rise to a wave backscattered during all the duration of the round-trip of the pulse in the fiber, i.e. during a duration of 2×L/c.
A second acousto-optical modulator MAO2 is provided at the output of the circulator C, as is a coupler CPL in order to divide the output pulses into two channels. Means Dm allowing a length delay ΔL corresponding to the time taken by the light to make the round-trip through the sensing zone ΔL/2 are inserted into one of the two channels. This delay allows, on the video camera CA and the liquid-crystal spatial light modulator SLM, interference to be created between a wave and itself shifted in time.
This time shift corresponds to a distance shift of length ΔL/2 in the sensor. The wave that passes through the delayed channel originates from the position Ai in the fiber, and the wave that passes through the non-delayed channel originates from the position Bi in the fiber, which is located ΔL/2 further on in the sensor.
Interference of the backscatters originating from the positions Ai and Bi gives the phase difference between the backscatter coming from Ai and the backscatter coming from Bi. It is a question of the phase seen by the wave issued from the position Bi over the length ΔL/2. The decorrelation between the interference patterns corresponding to the N sensing zones in the sensor increases as sensing zone length increases.
Since the relative phase of N interference patterns is random, their superposition may decrease contrast and blur the fringes. This is why an acousto-optical modulator MAO2 may be inserted before the point where the backscatter is split into two channels by a coupler CPL. It allows a window of 2×ΔL duration to be opened in order to let interfere only waves originating from one sensing zone at a time.
In this case, one of the two channels serves as a reference with reference output optical pulses Ipri and the other channel serves as a signal channel carrying signal optical pulses IpsiS, all of which pulses are issued from output optical pulses Ipsi, the optical waves of the two channels interfere at the video camera and at the liquid-crystal spatial light modulator SLM.
This architecture allows, along the fiber, the phase perturbation induced by the physical quantity to be measured to be located with a spatial resolution of ΔL/2. It is measured by analyzing the frequency of the electrical signal delivered by the photodiode PD.
The maximum time between interrogation of two different sensing zones of the sensor is limited by the “turn-off” response time of the liquid crystals: i.e. toff, the reset time of the liquid crystals, in the liquid-crystal spatial light modulator SLM, this implying that the time between two successive pulses defined by the parameter tR must be greater than the parameter toff.
It is recommended to wait until the liquid crystals involved in the inscription of the interference pattern of the first sensing zone are once again available.
This exemplary embodiment comprises a distributed architecture based on the use of a dynamic Brillouin grating as a mobile reflector and of an optical interrogation wave comprising a series of optical pulses.
The Brillouin grating, which is generated by the interaction between two optical pulses, allows a sensing optical-fiber section to be defined. In this case, the frequency aspect of the stimulated Brillouin interaction is not of interest but only the reflection coefficient of the dynamic grating. A probe wave then allows the optical fiber to be probed.
The proposed architecture is schematically shown in
The Stokes wave is shifted toward low frequencies by ωB, the Brillouin frequency, corresponding to the Doppler effect: reflection of the pump from a mobile grating. This grating, equivalent to a Bragg grating (due to the electrostriction effect between the pump wave and the Stoke wave in silica) propagates in the same direction as the pump at the speed of sound cac in the fiber ωB=2ncac/λ.
The duration of the pulses determines the length of the grating. The grating is inscribed in succession at various positions Zr in the fiber.
Its position (i.e. the zone in the fiber where the reflection of the pulse at ωs crosses the pulse at ωp) is controlled by the time interval Δt between the two pulses. In practice, it is proposed to use a reflective treatment M at the end of the fiber in order to obtain the reflection of the wave at ωs, allowing the Brillouin scattering to be stimulated.
Thus, in the first channel, the first acousto-optical modulator MOA3 is used to obtain the pump pulses. In the second channel, the frequency of the laser is shifted by a value corresponding to ωB (ωs=ωp−ωs) i.e. about 10 GHz in optical fibres, then another acousto-optical modulator MAO4 is used to obtain the Stoke pulses.
A “probe” third wave issued from the optical assembly comprising a laser SL1 is injected into the fiber at a frequency ωs and makes a round-trip between the input of the fiber and the Brillouin grating RBi. It accumulates a phase shift on this round-trip.
This phase shift is the signal of interest. A hologram is generated on the liquid-crystal spatial light modulator SLM and on the video camera between the return of the probe and a reference originating from the same laser. An optical assembly is used comprising a laser SL1 that emits a laser beam, divided to generate a laser beam Fr, the other portion of said beam being inserted into an acousto-optical modulator to generate a series of pulses Ipi at the optical frequency ωs in order to carry out the reading step. Typically, the lifetime of the grating thus inscribed is defined by the lifetime of the acoustic phonons in the material of the optical fiber, which may as is conventionally the case be silica, i.e. about 10 ns. It is therefore necessary to read the phase in the 10 ns following the writing. The pulses Ipi inserted into the optical fiber generate, on output from the fiber, pulses IpsiS after reflection from the Brillouin grating RBi, these interfering with the reference beam on the video camera and SLM.
In each reading-writing cycle, the spectrum obtained in the cycle N is subtracted from the spectrum obtained in the cycle N+1 in order to access the information that is generated in the fiber section corresponding to the (read/write) interrogation by the pulses of the cycle N.
The period of the reading-writing process is:
T=2L/c=1/frep.
The spectrum Si(t, L−Zr) of the signal perturbing the phase at ti=i*T, for the Brillouin reflector RBi at the position L−Zri, is obtained. More precisely, Si(t, L−Zr) is the spectrum of the acoustic signal that modulates the phase in a return trip between the input of the fiber and the inscribed Brillouin reflector RBi, and therefore over the length 2×L−Zri.
| Number | Date | Country | Kind |
|---|---|---|---|
| 15 00033 | Jan 2015 | FR | national |
| Filing Document | Filing Date | Country | Kind |
|---|---|---|---|
| PCT/EP2016/050304 | 1/8/2016 | WO | 00 |
| Publishing Document | Publishing Date | Country | Kind |
|---|---|---|---|
| WO2016/110581 | 7/14/2016 | WO | A |
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|---|---|---|---|
| 4320475 | Leclerc | Mar 1982 | A |
| 4536861 | Graindorge | Aug 1985 | A |
| 20110320147 | Brady | Dec 2011 | A1 |
| Number | Date | Country |
|---|---|---|
| 3 013 449 | May 2015 | FR |
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| Number | Date | Country | |
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| 20180003551 A1 | Jan 2018 | US |
