WO2015176362A1 - 光脉冲压缩反射装置 - Google Patents
光脉冲压缩反射装置 Download PDFInfo
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- WO2015176362A1 WO2015176362A1 PCT/CN2014/081331 CN2014081331W WO2015176362A1 WO 2015176362 A1 WO2015176362 A1 WO 2015176362A1 CN 2014081331 W CN2014081331 W CN 2014081331W WO 2015176362 A1 WO2015176362 A1 WO 2015176362A1
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- optical
- pulse compression
- output
- pulse
- modulator
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01M—TESTING STATIC OR DYNAMIC BALANCE OF MACHINES OR STRUCTURES; TESTING OF STRUCTURES OR APPARATUS, NOT OTHERWISE PROVIDED FOR
- G01M11/00—Testing of optical apparatus; Testing structures by optical methods not otherwise provided for
- G01M11/30—Testing of optical devices, constituted by fibre optics or optical waveguides
- G01M11/31—Testing of optical devices, constituted by fibre optics or optical waveguides with a light emitter and a light receiver being disposed at the same side of a fibre or waveguide end-face, e.g. reflectometers
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01M—TESTING STATIC OR DYNAMIC BALANCE OF MACHINES OR STRUCTURES; TESTING OF STRUCTURES OR APPARATUS, NOT OTHERWISE PROVIDED FOR
- G01M11/00—Testing of optical apparatus; Testing structures by optical methods not otherwise provided for
- G01M11/30—Testing of optical devices, constituted by fibre optics or optical waveguides
- G01M11/31—Testing of optical devices, constituted by fibre optics or optical waveguides with a light emitter and a light receiver being disposed at the same side of a fibre or waveguide end-face, e.g. reflectometers
- G01M11/3109—Reflectometers detecting the back-scattered light in the time-domain, e.g. OTDR
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01M—TESTING STATIC OR DYNAMIC BALANCE OF MACHINES OR STRUCTURES; TESTING OF STRUCTURES OR APPARATUS, NOT OTHERWISE PROVIDED FOR
- G01M11/00—Testing of optical apparatus; Testing structures by optical methods not otherwise provided for
- G01M11/30—Testing of optical devices, constituted by fibre optics or optical waveguides
- G01M11/31—Testing of optical devices, constituted by fibre optics or optical waveguides with a light emitter and a light receiver being disposed at the same side of a fibre or waveguide end-face, e.g. reflectometers
- G01M11/3109—Reflectometers detecting the back-scattered light in the time-domain, e.g. OTDR
- G01M11/3145—Details of the optoelectronics or data analysis
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01M—TESTING STATIC OR DYNAMIC BALANCE OF MACHINES OR STRUCTURES; TESTING OF STRUCTURES OR APPARATUS, NOT OTHERWISE PROVIDED FOR
- G01M11/00—Testing of optical apparatus; Testing structures by optical methods not otherwise provided for
- G01M11/30—Testing of optical devices, constituted by fibre optics or optical waveguides
- G01M11/31—Testing of optical devices, constituted by fibre optics or optical waveguides with a light emitter and a light receiver being disposed at the same side of a fibre or waveguide end-face, e.g. reflectometers
- G01M11/3109—Reflectometers detecting the back-scattered light in the time-domain, e.g. OTDR
- G01M11/3154—Details of the opto-mechanical connection, e.g. connector or repeater
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01M—TESTING STATIC OR DYNAMIC BALANCE OF MACHINES OR STRUCTURES; TESTING OF STRUCTURES OR APPARATUS, NOT OTHERWISE PROVIDED FOR
- G01M11/00—Testing of optical apparatus; Testing structures by optical methods not otherwise provided for
- G01M11/30—Testing of optical devices, constituted by fibre optics or optical waveguides
- G01M11/31—Testing of optical devices, constituted by fibre optics or optical waveguides with a light emitter and a light receiver being disposed at the same side of a fibre or waveguide end-face, e.g. reflectometers
- G01M11/3172—Reflectometers detecting the back-scattered light in the frequency-domain, e.g. OFDR, FMCW, heterodyne detection
Definitions
- the invention relates to the field of optical fiber sensing technology, in particular to an optical time domain reflection device based on pulse compression of a detection pulse.
- Light reflection technology has a wide range of applications in the field of optical fiber sensing.
- the basic principle is: launching a beam of probe light into the fiber to be tested, and then passing through the photodetector to obtain the intensity curve of the backscattered light, thereby analyzing the fiber to be tested. Information on loss, breakpoints, etc.
- the traditional optical time domain reflection technique uses light pulses as the probe light, and its spatial resolution is determined by the pulse width. The narrower the pulse width, the higher the spatial resolution.
- optical frequency domain reflection technology In order to break through the bottleneck of traditional optical time domain reflection technology, optical frequency domain reflection technology has been proposed.
- the optical frequency domain reflection technique uses linearly modulated continuous light as the probe light, and there is a phase difference between the optical signal reflected from different positions in the optical fiber and the linear frequency modulated continuous light to form optical beat signals of different frequency differences. After being converted into photocurrent by the photodetector, the optical fiber reflection information can be obtained by transforming into the frequency domain.
- the spatial resolution of the optical frequency domain reflection technique is only determined by the range of the chirp, so there is no spatial resolution and detection range mutually constrained. However, the detection range of the optical frequency domain reflection technique is limited by the coherence length of the light source.
- the maximum detection range is about half of the coherence length of the light source [D. Uttam and B. Culshaw, "Precision time Domain reflectometry in optical fiber systems using a frequency modulated continuous wave ranging technique, "oarna/ of Lightwave Technology, wo ⁇ . 3, no. 5, pp. 971-977, 1985].
- pulse compression radar technology to optical time domain reflection technology can not only break the contradiction between the spatial resolution and detection range of traditional optical time domain reflection technology, but also exert the ultra-high spatial resolution of pulse compression technology.
- Optical frequency domain reflection technology has a larger detection range.
- an object of the present invention to provide an optical pulse compression and reflection device that achieves a higher spatial resolution than conventional optical time domain reflection techniques and a larger detection range than optical frequency domain reflection techniques.
- An optical pulse compression reflection device comprising: a single wavelength continuous light source, a beam splitter, a frequency modulation pulse generation module, an optical directional coupler, an optical fiber to be tested, an optical coupler, a balanced photodetector, and a pulse compression processing module;
- An output end of the single-wavelength continuous light source is connected to an input end of the optical splitter, and a first output end of the optical splitter is connected to a first port of the optical directional coupler via the FM pulse generating module a second port of the optical directional coupler is coupled to the optical fiber to be tested, a third port of the optical directional coupler is coupled to the first input end of the optical coupler, and a second of the optical splitter The output end is connected to the second input end of the optical coupler;
- the two outputs of the optical coupler are connected to the balanced photodetector, and the output of the balanced photodetector is connected to the pulse compression processing module.
- the first embodiment of the FM pulse generating module includes: a polarization controller, a chirped voltage controlled oscillator, a waveform generator, a single sideband modulator, a polarization controller, an erbium doped fiber amplifier, and a Mach-Zengde electro-optic modulator And erbium doped fiber amplifiers;
- the second embodiment of the FM pulse generating module includes: a polarization controller, a linear frequency modulation voltage controlled oscillator, a waveform generator, a single sideband modulator, and an erbium doped fiber amplifier;
- the wave output end of the waveform generator is connected to the input end of the linear frequency modulation voltage controlled oscillator, and the output end of the linear frequency modulation voltage controlled oscillator is connected to the electrical signal input end of the single sideband modulator a first output of the beam splitter via the polarization controller and an input of the single sideband modulator Connected, the output of the single sideband modulator is sequentially connected to the input end of the Mach-Zehnder electro-optic modulator via the polarization controller and the erbium-doped fiber amplifier, and the pulse output of the waveform generator Connected to the electrical signal input of the Mach-Zehnder electro-optic modulator, the output of the Mach-Zehnder electro-optic modulator is connected to the input of the optical directional coupler via the erbium-doped fiber amplifier.
- the Mach-Zehnder electro-optic modulator is a light intensity modulator, a single sideband modulator or an electroabsorption modulator.
- the pulse compression processing module includes a data collector, a quadrature demodulator and a matched filter connected in sequence;
- the data collector collects an electrical signal output by the balanced photodetector, and the quadrature demodulator performs orthogonal demodulation on the collected signal; the matched filter will have an orthogonal solution
- the adjusted signal is matched for filtering.
- the data collector is an analog receiving circuit, an analog to digital conversion module, a data acquisition card or an oscilloscope.
- the pulse compression processing module is an analog signal processing circuit, a digital signal processor or computer software.
- the single-wavelength continuous light source is a semiconductor laser, a fiber laser, a bulk laser or a dye laser.
- the optocoupler is a 2x2 optocoupler.
- the balanced photodetector is a PIN diode or an APD avalanche photodiode.
- the optical directional coupler is an optical circulator or an optical coupler.
- the light source is divided into two paths, one is used as the reference light for coherent detection, and one pulse is generated as the probe light, which is compressed into a narrow pulse in the time domain by pulse compression processing, and the compression ratio is only related to the frequency modulation range and the light pulse width. .
- the monochromatic continuous optical signal generated by the single-wavelength continuous light source is split by the optical splitter; the FM pulse generating module converts the split optical signal into the modulated optical pulse as the probe light; and one end of the optical directional coupler detects the light from the other After one end is output to the optical fiber to be tested, the generated backscattered light or reflected light is output through the optical directional coupler; one input end of the optical coupler is connected to the backscattered light, and the other light split by the optical splitter As a reference light, another segment of the optical coupler is connected; the two outputs of the optical coupler are connected to the balanced photodetector for performing the coherent detection; and the pulse compression processing module performs the pulse for the signal obtained by the coherent detection Compression processing.
- the present invention has the following advantages:
- the principle of pulse compression breaks through the limitation between the spatial resolution and the detection range of the traditional optical time domain reflection technique, and at the same time, it has a larger detection range than the optical frequency domain reflection technique.
- FIG. 1 is a schematic structural view of an optical pulse compression reflection device of the present invention.
- FIG. 2 is a schematic diagram of pulse compression processing of the optical pulse compression reflection device of the present invention, wherein (a) is a primary pulse; (b) is a compressed pulse.
- FIG. 3 is a schematic structural view of a first embodiment of a frequency modulated optical pulse generating module in an optical pulse compression and reflection device according to the present invention.
- FIG. 4 is a schematic structural view of a second embodiment of a frequency modulated optical pulse generating module in an optical pulse compression and reflection device according to the present invention.
- FIG. 5 is a schematic structural diagram of a pulse compression processing module in an optical pulse compression and reflection device according to the present invention.
- FIG. 6 is an experimental result of the optical pulse compression and reflection device of the present invention in a specific embodiment of the frequency modulated light pulse generating module, wherein (a) is a backscattering curve; (b) is a spatial resolution verification. (Experimental conditions, pulse width 2 s, frequency modulation range 221 MHz, laser source line width 100 kHz, spatial resolution of approximately 50 cm, test range 5.4 km).
- FIG. 1 is a schematic structural view of an optical pulse compression and reflection device according to the present invention.
- the basic configuration includes: a single wavelength continuous light source 1, a beam splitter 2, a frequency modulation pulse generation module 3, an optical directional coupler 5, and an optical fiber to be tested 6 , optical coupler 9, balanced photodetector 10, pulse compression processing module 11;
- the connection relationship of the above components is as follows:
- the monochromatic continuous optical signal generated by the single-wavelength continuous light source 1 is split by the optical splitter 2; the FM pulse generating module 3 converts the optical signal of the split light into a modulated optical pulse as the probe light 4,
- the first port of the optical directional coupler 5 receives the probe light 4 and outputs it from the second port to the optical fiber 6 to be tested, and the second port of the optical directional coupler 5 receives the test.
- the backscattered light produced by the fiber 6 is output from the third port.
- the second input end of the optical coupler 9 receives the backscattered light, and the other light split by the splitter 2 is used as the reference light 7 to access the first input end of the optical coupler 9;
- the two outputs of the optocoupler 9 are connected to the balanced photodetector 10 for coherent detection; the pulse compression processing module 11 performs pulse compression processing on the signal output by the balanced photodetector 10.
- using indicates a chirp signal, and ) indicates a pulse-compressed signal.
- ⁇ is the pulse amplitude
- ⁇ is the pulse width
- ⁇ is the frequency modulation rate
- r « () represents the rectangular function.
- Fig. 2 is a schematic diagram showing the simulation of the above process, i.e., the pulse compression processing diagram of the pulse compression light reflecting system of the present invention, (a) being the original pulse and (b) being the compressed pulse.
- the spatial resolution ⁇ can be defined as the minimum resolvable event distance, and the time domain reflection method is equal to the product of the detected pulse width and the speed of light in the medium.
- the spatial resolution of the pulse compression light reflecting system of the present invention is only related to the frequency modulation range ⁇ ,
- c is the speed of light in the vacuum and w is the refractive index of the medium.
- the detection range of the system can be defined as the maximum detection distance that keeps the event signal power greater than the noise power, which increases with the increase of the pulse width in the time domain reflection method. Since the spatial resolution of the pulse compression light reflection system of the present invention is only related to the frequency modulation range ⁇ , and is independent of the pulse width, the pulse compression light reflection system of the present invention can greatly increase the pulse width by maintaining high spatial resolution. Improve the detection range. In addition, it can be seen from Figure 2 that by pulse compression, the originally evenly distributed energy is concentrated in very In a short period of time, the instantaneous power of the reflected signal at the event is increased, the signal-to-noise ratio is improved, and the detection range is further improved.
- the FM optical pulse generation module includes: a polarization controller 12, a linear frequency modulation voltage controlled oscillator 13, and a waveform.
- Generator 14 single sideband modulator 15, polarization controller 16, erbium doped fiber amplifier 17, Mach-Zehnder electro-optic modulator 18 and erbium doped fiber amplifier 19.
- the connection relationship between the components of the FM pulse generation module is as follows:
- the waveform generator 14 generates a periodic sawtooth wave to drive the linear frequency modulation voltage controlled oscillator 13, and oscillates the linear frequency modulation voltage control
- the output end of the device 13 is connected to the electrical signal input end of the single sideband modulator 15; then, a light obtained by the splitter 2 is passed through the polarization controller 12 and then connected to the a single sideband modulator 15; the output light of the single sideband modulator 15 is passed through the polarization controller 16 and the erbium doped fiber amplifier 17 to the Mach-Zehnder electro-optic modulator 18
- the waveform generator generates a pulse synchronized with the periodic sawtooth wave to enter the electrical signal input end of the Mach-Zehnder electro-optic modulator 18; the output of the Mach-Zehnder electro-optic modulator 18
- the probe light 4 is generated after the light passes through the erbium doped fiber amplifier 19.
- the FM optical pulse generating module includes: a waveform generator 20, a linear frequency modulation voltage controlled oscillator 21, and a polarization. Controller 22, single sideband modulator 23 and erbium doped fiber amplifier 24.
- the connection relationship between the components of the FM pulse generation module is as follows: The waveform generator 20 generates two signals, one is a periodic sawtooth wave, and the electrical signal input of the linear frequency modulation voltage controlled oscillator 21 is connected.
- the other end is a periodic pulse signal having a pulse width equal to the periodic sawtooth period and is connected to the enable input of the chirped voltage controlled oscillator 21.
- the output of the chirped voltage controlled oscillator 13 is connected to the electrical signal input end of the single sideband modulator 23; then, a light split by the splitter 2 passes through the polarization
- the controller 22 is then connected to the single sideband modulator 23; the output light of the single sideband modulator 23 is passed through the erbium doped fiber amplifier 24 to generate the probe light 4.
- FIG. 5 is a schematic structural diagram of a pulse compression processing module in an optical pulse compression and reflection device according to the present invention.
- the pulse compression processing module includes a data collector 25, a quadrature demodulator 26, and a matched filter 27 which are sequentially connected.
- the data collector 25 collects the electrical signals output by the coherent detection 8
- the quadrature demodulator 26 performs quadrature demodulation on the collected signal; the matched filter 27 performs matched filtering on the quadrature demodulated signal.
- a linearly swept continuous wave is output due to being driven by a periodic sawtooth wave.
- a single sideband modulator it modulates the input electrical signal only to the upper or lower sideband of the light, so the frequency of the output light is linear with the frequency of the input electrical signal, in a specific implementation of the frequency modulated optical pulse generation module After the linear frequency-swept continuous light wave generated by the above-mentioned linear frequency modulation voltage controlled oscillator is connected, the single sideband modulator generates a linear frequency sweeping continuous light.
- the linearly swept continuous light is passed through the above-mentioned Mach-Zehnder electro-optic modulator to modulate a pulse synchronized with the periodic sawtooth wave to obtain a linearly swept optical pulse; in the second embodiment of the FM optical pulse generating module
- the pulse synchronized with the periodic sawtooth wave is connected to the enable end of the above-mentioned linear frequency modulation voltage controlled oscillator, and the linear frequency modulation voltage controlled oscillator directly generates a linear frequency sweeping electric pulse, so the above-mentioned linear frequency modulation voltage controlled oscillator After the generated linear swept electrical pulse is applied, the single sideband modulator directly generates a linearly swept optical pulse.
- the optical fiber coupler is used to interfere with the backward reflected light of the optical fiber and the reference light, and then the coherent detection is realized by the balanced photodetector to obtain the optical electric field and the frequency modulation information.
- the obtained real signal can be converted into a complex signal by orthogonal demodulation, and the signal center frequency is shifted down to the intermediate frequency or zero point, and then matched and filtered to achieve pulse compression while greatly improving.
- the signal to noise ratio of the reflected signal is used to interfere with the backward reflected light of the optical fiber and the reference light, and then the coherent detection is realized by the balanced photodetector to obtain the optical electric field and the frequency modulation information.
- the obtained real signal can be converted into a complex signal by orthogonal demodulation, and the signal center frequency is shifted down to the intermediate frequency or zero point, and then matched and filtered to achieve pulse compression while greatly improving.
- the signal to noise ratio of the reflected signal is used to interfere with the backward reflected light of the optical fiber and the reference light, and
Abstract
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Priority Applications (3)
Application Number | Priority Date | Filing Date | Title |
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US14/443,916 US9689772B2 (en) | 2014-05-19 | 2014-07-01 | Optical pulse compression reflectometer |
EP14870645.0A EP3098651B1 (en) | 2014-05-19 | 2014-07-01 | Light pulse compression reflectometer |
JP2016520269A JP2016524715A (ja) | 2014-05-19 | 2014-07-01 | 光パルス圧縮反射装置 |
Applications Claiming Priority (2)
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CN201410211203.5A CN103984184B (zh) | 2014-05-19 | 2014-05-19 | 光脉冲压缩反射装置 |
CN201410211203.5 | 2014-05-19 |
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PCT/CN2014/081331 WO2015176362A1 (zh) | 2014-05-19 | 2014-07-01 | 光脉冲压缩反射装置 |
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US (1) | US9689772B2 (zh) |
EP (1) | EP3098651B1 (zh) |
JP (1) | JP2016524715A (zh) |
CN (1) | CN103984184B (zh) |
WO (1) | WO2015176362A1 (zh) |
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CN106571880A (zh) * | 2016-10-21 | 2017-04-19 | 北京无线电计量测试研究所 | 一种太赫兹器件传输参数的测量系统与方法 |
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EP3098651A1 (en) | 2016-11-30 |
US20160245719A1 (en) | 2016-08-25 |
US9689772B2 (en) | 2017-06-27 |
CN103984184B (zh) | 2016-08-24 |
EP3098651B1 (en) | 2020-06-03 |
JP2016524715A (ja) | 2016-08-18 |
CN103984184A (zh) | 2014-08-13 |
EP3098651A4 (en) | 2017-04-12 |
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