CN104180910A - Spectral width measuring device and method used for SLED light source - Google Patents

Spectral width measuring device and method used for SLED light source Download PDF

Info

Publication number
CN104180910A
CN104180910A CN201410476577.XA CN201410476577A CN104180910A CN 104180910 A CN104180910 A CN 104180910A CN 201410476577 A CN201410476577 A CN 201410476577A CN 104180910 A CN104180910 A CN 104180910A
Authority
CN
China
Prior art keywords
light source
photodetector
optical fiber
formula
sled
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
CN201410476577.XA
Other languages
Chinese (zh)
Inventor
吴东方
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
SUZHOU GUANGLAN INFORMATION TECHNOLOGY Co Ltd
Original Assignee
SUZHOU GUANGLAN INFORMATION TECHNOLOGY Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by SUZHOU GUANGLAN INFORMATION TECHNOLOGY Co Ltd filed Critical SUZHOU GUANGLAN INFORMATION TECHNOLOGY Co Ltd
Priority to CN201410476577.XA priority Critical patent/CN104180910A/en
Publication of CN104180910A publication Critical patent/CN104180910A/en
Pending legal-status Critical Current

Links

Abstract

The invention discloses a spectral width measuring device and method used for an SLED light source. The device comprises the SLED light source to be measured, a first photoelectric detector, a second photoelectric detector, a third photoelectric detector, an optical fiber circulator, a 3*3 optical fiber coupler, an online luminous power meter, a first 2*2 optical fiber coupler, a second 2*2 optical fiber coupler, an optical fiber lithium niobate phase modulator, a first Faraday rotary reflector, a delay optical fiber cable, a second Faraday rotary reflector and a data terminal. The number of light paths used for measuring the spectral width of the SLED light source is at least two, and interference exists between the two two-beam light paths. The spectral width measuring device and method used for the SLED light source can quickly and accurately measure the spectral width of the SLED light source, are low in cost and convenient to use and have good application prospects.

Description

A kind of spectrum width measurement mechanism and method for SLED light source
Technical field
The present invention relates to a kind of spectrum width measurement mechanism and method for SLED light source, belong to spectral signature field of measuring technique.
Background technology
Along with the developing rapidly of optical fiber sensing technology, fibre optic gyroscope, fibre optic hydrophone, optical fiber sensing security system be the corresponding application obtaining more extensively and profoundly also in recent years, from before single Military Application develop into present civil area.
Due to the applied concrete know-why difference of these optical fiber sensing systems, the LASER Light Source kind using is also different, only taking optical fiber sensing security system as example, applied just have M-Z, sagnac, many technology paths of OTDR, thereby related LASER Light Source has the polytypes such as DFB-LD type, fiber laser, ASE light source.But, because low relevant wide spectrum light source can suppress interference and the negative effect that in optical fiber, Rayleigh scattering and Kerr effect etc. are brought preferably, thereby fibre optic gyroscope based on wide range LASER Light Source technology, optical fiber sensing security system, fibre optic hydrophone in Fibre Optical Sensor in occupation of more and more important share, the special LASER Light Source that can use hardly other type in the application of fibre optic gyroscope except using wide range LASER Light Source.SLED light source is a kind of most typical wide range LASER Light Source.
But, the spectrum width of LASER Light Source is not more wide better yet, but just can reach within the specific limits optimum efficiency, taking fibre optic gyroscope as example, light source spectrum width is wider in theory, and its effect that suppresses measuring error can be better, but widely can produce harmful effect to the linearity of system scale factor, stability again, therefore, select the SLED light source of suitable spectrum width extremely important, need a kind of device that can accurately measure SLED spectrum width to select SLED light source for this reason.Certainly, use fiber spectrometer can realize this purpose, and can obtain other physical characteristic parameter of LASER Light Source, but problem is, at present, fiber spectrometer price is still very expensive, and other detailed physical features that we do not need to obtain LASER Light Source in this type of application of fibre optic gyroscope is as ripple feature etc., can measure the spectrum width of all laser class light sources does not in fact also pay close attention to fiber spectrometer, thereby, be badly in need of a kind of with low cost, can Quick Measurement the device of SLED type LASER Light Source spectrum width, solve the problems referred to above.
Summary of the invention
The object of the invention is to overcome existing fiber spectrometer expensive, be difficult to penetration and promotion to measure the spectrum width of SLED light source, spectrum width measurement mechanism and method for SLED light source of the present invention, can accurately measure fast the spectrum width of SLED light source, with low cost, easy to use, have a good application prospect.
In order to achieve the above object, the technical solution adopted in the present invention is:
A kind of spectrum width measurement mechanism for SLED light source, it is characterized in that: comprise SLED light source to be measured, the first photodetector, the second photodetector, the 3rd photodetector, optical fiber circulator, 3 × 3 fiber couplers, luminous power on-line measurement meter, the one 2 × 2 fiber coupler, the 22 × 2 fiber coupler, optical fiber lithium niobate phase modulator, the first faraday rotator mirror, postpone optical fiber cable, the second faraday rotator mirror and data terminal
Described SLED light source to be measured, the second photodetector is connected with 3 × 3 fiber couplers by optical fiber circulator respectively, described the first photodetector, the 3rd photodetector is connected with 3 × 3 fiber couplers respectively, described 3 × 3 fiber couplers respectively with the one 2 × 2 fiber coupler, the 22 × 2 fiber coupler is connected, described the one 2 × 2 fiber coupler is connected with the first faraday rotator mirror by optical fiber lithium niobate phase modulator, described the 22 × 2 fiber coupler is connected with the second faraday rotator mirror by postponing optical fiber cable, described the one 2 × 2 fiber coupler, the 22 × 2 fiber coupler is connected by optical fiber, described 3 × 3 fiber couplers are also connected with luminous power on-line measurement meter, described the first photodetector, the second photodetector, the 3rd photodetector is connected with data terminal respectively by cable.
Aforesaid a kind of spectrum width measurement mechanism for SLED light source, is characterized in that: be at least two for measuring the light path approach of SLED light source spectrum width, and exist two two-beam roads to interfere.
The measuring method of a kind of spectrum width measurement mechanism for SLED light source based on above-mentioned, is characterized in that: comprises the following steps,
Step (1), exports three road interference lights by data terminal control the first photodetector, the second photodetector, the 3rd photodetector, makes adjacent two-way interference light have the phase differential of 120 ° by 3 × 3 fiber couplers;
Step (2), modulates by optical fiber lithium niobate phase modulator the phase differential that three road interference lights cause in external disturbance
Step (3), according to formula (1), calculates interference light intensity
Wherein, i (k) is spectral concentration function; K is the wave number of interference light, k=2 π/λ, and λ is for interfering light wavelength;
Step (4), according to formula (2), (3), calculates the spectral concentration function i (k) of SLED light source,
Δk/k=Δλ/λ (2)
i ( k ) = 1 πΔk e - ( k - k 0 Δk ) 2 - - - ( 3 )
Wherein, Δ λ is the spectrum width of SLED light source, and Δ k is the increment of wave number k,
∫ - ∞ ∞ i ( k ) dk = I 0
Wherein, I 0for the light intensity of SLED light source;
Step (5), according to improper integral formula (4),
∫ - ∞ ∞ cos ax · e ( - bx 2 ) dx = π b e ( - a 2 4 b ) - - - ( 4 )
Wherein, formula (4) is improper integral formula, and a, b are constant;
Step (6), brings formula (1) into according to formula (2), formula (3), formula (4), obtains formula (5),
Step (7), according to formula (5), obtains the spectrum width Δ λ of SLED light source,
The invention has the beneficial effects as follows: spectrum width measurement mechanism and method for SLED light source of the present invention, can accurately measure fast the spectrum width of SLED light source, with low cost, easy to use, have a good application prospect.
Brief description of the drawings
Fig. 1 is the system chart of the spectrum width measurement mechanism for SLED light source of the present invention.
Fig. 2 is the process flow diagram of the spectrum width measuring method for SLED light source of the present invention.
Fig. 3 is the spectrogram of SLED light source of the present invention.
Embodiment
Below in conjunction with Figure of description, the invention will be further described.Following examples are only for technical scheme of the present invention is more clearly described, and can not limit the scope of the invention with this.
As shown in Figure 1, solid line is optical fiber; Dotted line is cable, spectrum width measurement mechanism for SLED light source of the present invention, comprise SLED light source 1 to be measured, the first photodetector 2, the second photodetector 3, the 3rd photodetector 4, optical fiber circulator 5,3 × 3 fiber couplers 6, luminous power on-line measurement meter the 7, the one 2 × 2 fiber coupler the 8, the 22 × 2 fiber coupler 9, optical fiber lithium niobate phase modulator 10, the first faraday rotator mirror 11, postpone optical fiber cable 12, the second faraday rotator mirror 13 and data terminal 14
Described SLED light source 1 to be measured, the second photodetector 3 is connected with 3 × 3 fiber couplers 6 by optical fiber circulator 5 respectively, the first photodetector 2, the 3rd photodetector 4 is connected with 3 × 3 fiber couplers 6 respectively, 3 × 3 fiber couplers 6 respectively with the one 2 × 2 fiber coupler 8, the 22 × 2 fiber coupler 9 is connected, the one 2 × 2 fiber coupler 8 is connected with the first faraday rotator mirror 11 by optical fiber lithium niobate phase modulator 10, the 22 × 2 fiber coupler 9 is connected with the second faraday rotator mirror 13 by postponing optical fiber cable 12, the one 2 × 2 fiber coupler 8, the 22 × 2 fiber coupler 9 is connected by optical fiber, 3 × 3 fiber couplers 6 are also connected with luminous power on-line measurement meter 7, the first photodetector 2, the second photodetector 3, the 3rd photodetector 4 is connected with data terminal 14 respectively by cable.
Wherein 3 × 3 fiber couplers 6 have the phase bias characteristic of 120 degree, thus between the light splitting of 3 road interference lights of input, there is the phase differential of 120 degree, can be by the phase differential of interference light by 3 road interference light signals demodulation out, then continues to calculate the spectrum width of SLED light source 1.
Be at least two for the light path approach of measuring SLED light source 1 spectrum width, and exist two two-beam roads to interfere, as shown in Figure 1, can form light path approach has 6,
1)1-5-6-8-10-11-10-8-9-12-13-12-9-6;
2)1-5-6-9-12-13-12-9-8-10-11-10-8-6;
3)1-5-6-8-10-11-10-8-6;
4)1-5-6-9-12-13-12-9-6;
5)1-5-6-8-10-11-10-8-9-12-13-12-9-8-10-11-10-8-6;
6)1-5-6-9-12-13-12-9-8-10-11-10-8-9-12-13-12-9-6;
6 above-mentioned light path approach, as long as there are two two-beam roads of existence to interfere.
As shown in Figure 2, the measuring method of the spectrum width measurement mechanism for SLED light source based on above-mentioned, comprises the following steps,
Step (1), control the first photodetector (2), the second photodetector (3), the 3rd photodetector (4) output three road interference lights by data terminal (14), make adjacent two-way interference light have the phase differential of 120 ° by 3 × 3 fiber couplers (6);
Step (2), modulates by optical fiber lithium niobate phase modulator (10) phase differential that three road interference lights cause in external disturbance
Step (3), according to formula (1), calculates interference light intensity
Wherein, i (k) is spectral concentration function; K is the wave number of interference light, k=2 π/λ, and λ is for interfering light wavelength;
Step (4), according to the spectral concentration function i (k) of formula (2), (3) calculating SLED light source, the spectrogram of SLED light source, as shown in Figure 3,
Δk/k=Δλ/λ (2)
i ( k ) = 1 πΔk e - ( k - k 0 Δk ) 2 - - - ( 3 )
Wherein, Δ λ is the spectrum width of SLED light source, and Δ k is the increment of wave number k,
∫ - ∞ ∞ i ( k ) dk = I 0
Wherein, I 0for the light intensity of SLED light source;
Step (5), according to improper integral formula (4),
∫ - ∞ ∞ cos ax · e ( - bx 2 ) dx = π b e ( - a 2 4 b ) - - - ( 4 )
Wherein, formula (4) is improper integral formula, and a, b are constant;
Step (6), brings formula (1) into according to formula (2), formula (3), formula (4), obtains formula (5),
Step (7), according to formula (5), obtains the spectrum width Δ λ of SLED light source,
In sum, spectrum width measurement mechanism and method for SLED light source of the present invention, can accurately measure the spectrum width of SLED light source fast, with low cost, easy to use, has a good application prospect.
More than show and described ultimate principle of the present invention, principal character and advantage.The technician of the industry should understand; the present invention is not restricted to the described embodiments; that in above-described embodiment and instructions, describes just illustrates principle of the present invention; without departing from the spirit and scope of the present invention; the present invention also has various changes and modifications, and these changes and improvements all fall in the claimed scope of the invention.The claimed scope of the present invention is defined by appending claims and equivalent thereof.

Claims (3)

1. the spectrum width measurement mechanism for SLED light source, it is characterized in that: comprise SLED light source to be measured (1), the first photodetector (2), the second photodetector (3), the 3rd photodetector (4), optical fiber circulator (5), 3 × 3 fiber couplers (6), luminous power on-line measurement meter (7), the one 2 × 2 fiber coupler (8), the 22 × 2 fiber coupler (9), optical fiber lithium niobate phase modulator (10), the first faraday rotator mirror (11), postpone optical fiber cable (12), the second faraday rotator mirror (13) and data terminal (14),
Described SLED light source to be measured (1), the second photodetector (3) is connected with 3 × 3 fiber couplers (6) by optical fiber circulator (5) respectively, described the first photodetector (2), the 3rd photodetector (4) is connected with 3 × 3 fiber couplers (6) respectively, described 3 × 3 fiber couplers (6) respectively with the one 2 × 2 fiber coupler (8), the 22 × 2 fiber coupler (9) is connected, described the one 2 × 2 fiber coupler (8) is connected with the first faraday rotator mirror (11) by optical fiber lithium niobate phase modulator (10), described the 22 × 2 fiber coupler (9) is connected with the second faraday rotator mirror (13) by postponing optical fiber cable (12), described the one 2 × 2 fiber coupler (8), the 22 × 2 fiber coupler (9) is connected by optical fiber, described 3 × 3 fiber couplers (6) are also connected with luminous power on-line measurement meter (7), described the first photodetector (2), the second photodetector (3), the 3rd photodetector (4) is connected with data terminal (14) respectively by cable.
2. a kind of spectrum width measurement mechanism for SLED light source according to claim 1, is characterized in that: be at least two for measuring the light path approach of SLED light source spectrum width, and exist two two-beam roads to interfere.
3. the measuring method based on a kind of spectrum width measurement mechanism for SLED light source claimed in claim 1, is characterized in that: comprises the following steps,
Step (1), control the first photodetector (2), the second photodetector (3), the 3rd photodetector (4) output three road interference lights by data terminal (14), make adjacent two-way interference light have the phase differential of 120 ° by 3 × 3 fiber couplers (6);
Step (2), modulates by optical fiber lithium niobate phase modulator (10) phase differential that three road interference lights cause in external disturbance
Step (3), according to formula (1), calculates interference light intensity
Wherein, i (k) is spectral concentration function; K is the wave number of interference light, k=2 π/λ, and λ is for interfering light wavelength;
Step (4), according to formula (2), (3), calculates the spectral concentration function i (k) of SLED light source,
Δk/k=Δλ/λ (2)
i ( k ) = 1 πΔk e - ( k - k 0 Δk ) 2 - - - ( 3 )
Wherein, Δ λ is the spectrum width of SLED light source, and Δ k is the increment of wave number k,
∫ - ∞ ∞ i ( k ) dk = I 0
Wherein, I 0for the light intensity of SLED light source;
Step (5), according to improper integral formula (4),
∫ - ∞ ∞ cos ax · e ( - bx 2 ) dx = π b e ( - a 2 4 b ) - - - ( 4 )
Wherein, formula (4) is improper integral formula, and a, b are constant;
Step (6), brings formula (1) into according to formula (2), formula (3), formula (4), obtains formula (5),
Step (7), according to formula (5), obtains the spectrum width Δ λ of SLED light source,
CN201410476577.XA 2014-09-18 2014-09-18 Spectral width measuring device and method used for SLED light source Pending CN104180910A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201410476577.XA CN104180910A (en) 2014-09-18 2014-09-18 Spectral width measuring device and method used for SLED light source

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201410476577.XA CN104180910A (en) 2014-09-18 2014-09-18 Spectral width measuring device and method used for SLED light source

Publications (1)

Publication Number Publication Date
CN104180910A true CN104180910A (en) 2014-12-03

Family

ID=51962138

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201410476577.XA Pending CN104180910A (en) 2014-09-18 2014-09-18 Spectral width measuring device and method used for SLED light source

Country Status (1)

Country Link
CN (1) CN104180910A (en)

Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN1614455A (en) * 2004-12-02 2005-05-11 复旦大学 Optical fibre phase modulation and feedback white light interference system
CN1648700A (en) * 2005-04-05 2005-08-03 复旦大学 Method for structuring feedback delay of optical fiber line and full light fiber white light interference system made thereof
WO2005095918A2 (en) * 2004-03-29 2005-10-13 Carl Zeiss Meditec Inc. Simple high efficiency optical coherence domain reflectometer design
CN101183014A (en) * 2007-12-13 2008-05-21 北京理工大学 Full polarization-preserving fiber interferometer based on 3X3 polarization-preserving fiber coupling mechanism
US20080310791A1 (en) * 2007-06-14 2008-12-18 Yong Huang All-fiber current sensor
CN204154398U (en) * 2014-09-18 2015-02-11 苏州光蓝信息技术有限公司 A kind of spectrum width measurement mechanism for SLED light source

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2005095918A2 (en) * 2004-03-29 2005-10-13 Carl Zeiss Meditec Inc. Simple high efficiency optical coherence domain reflectometer design
CN1614455A (en) * 2004-12-02 2005-05-11 复旦大学 Optical fibre phase modulation and feedback white light interference system
CN1648700A (en) * 2005-04-05 2005-08-03 复旦大学 Method for structuring feedback delay of optical fiber line and full light fiber white light interference system made thereof
US20080310791A1 (en) * 2007-06-14 2008-12-18 Yong Huang All-fiber current sensor
CN101183014A (en) * 2007-12-13 2008-05-21 北京理工大学 Full polarization-preserving fiber interferometer based on 3X3 polarization-preserving fiber coupling mechanism
CN204154398U (en) * 2014-09-18 2015-02-11 苏州光蓝信息技术有限公司 A kind of spectrum width measurement mechanism for SLED light source

Non-Patent Citations (7)

* Cited by examiner, † Cited by third party
Title
曹茂永: "《矿用新型传感器》", 30 September 2011, 中国矿业大学出版社 *
杨圣: "《先进传感技术》", 31 January 2014, 中国科学技术大学出版社 *
杨淑芬: "《全光光纤通信网》", 31 January 2004, 科学出版社 *
江毅,唐才杰: "《光纤Fabry-Perot干涉仪原理及应用》", 30 April 2009, 国防工业出版社 *
舒建涛,季旭东,李绪友: "光源谱宽对干涉式光纤陀螺影响的分析", 《压电与声光》 *
董翔: "全光纤白光干涉仪在光谱测量中的应用", 《中国优秀硕士学位论文全文数据库工程科技II辑》 *
董翔: "全光纤白光干涉仪在光谱测量中的运用", 《中国优秀硕士学位论文全文数据库工程科技II辑》 *

Similar Documents

Publication Publication Date Title
CN102759371B (en) COTDR (coherent detection based optical time-domain reflectometry) fused long-distance coherent detection brilouin optical time-domain analyzer
CN100567919C (en) Collimation optical FMCW backscattering measuring system
CN104792343B (en) Brillouin light fiber sensor system and method for sensing that a kind of single-ended structure is dynamically measured
CN102798411B (en) System and method for distributed optical fibre sensing measurement based on Brillouin scattering
CN103091072B (en) Based on optical device measuring method, the measurement mechanism of optical SSB modulation
CN101713701B (en) Heterodyne technology based device and method for testing half-wave voltage of phase modulator
CN104677396A (en) Dynamic distributed Brillouin optical fiber sensing device and method
CN103344614B (en) A kind of atmospheric transmissivity at high precision measurement mechanism and measuring method
US9658052B2 (en) Method for reducing interference from scattered light/reflected light of interference path by generating carrier through phase
CN102914423B (en) Measuring method for sag frequency of dispersion optical fiber
CN103438882B (en) A kind of optical fibre gyro of low scale factor error
CN104132798A (en) Y-waveguide integrated optics phase modulator modulation factor measurement device and method
CN204439100U (en) Dynamic distributed Brillouin light fiber sensing equipment
CN101639387B (en) Optical fiber temperature sensor for detection based on wavelength corresponding to extreme value and temperature sensing method
CN102878953B (en) Precision angle method and device thereof
CN103414513B (en) A kind of pulsed light dynamic extinction ratio measurement mechanism and method with high dynamic range
CN104122423A (en) BGO (Bismuth Germanium Oxide) crystal electro-optic coefficient temperature relevancy self-compensation device and method
CN105203136A (en) Distributed sensing system based on differential amplification technology
CN103940501B (en) A kind of BOTDA distributed vibration sensing system based on dynamic phasing demodulation
CN106989904A (en) A kind of measuring method of polarization maintaining optical fibre extinction ratio
CN111678584A (en) Optical fiber vibration measuring device with light source frequency shift calibration auxiliary channel and method
CN204630588U (en) A kind of Brillouin light fiber sensor system of single-ended structure kinetic measurement
CN107976300B (en) Method for measuring beat length of polarization maintaining optical fiber
CN203758532U (en) Brillouin fiber-optic sensing system
CN204154398U (en) A kind of spectrum width measurement mechanism for SLED light source

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
RJ01 Rejection of invention patent application after publication

Application publication date: 20141203

RJ01 Rejection of invention patent application after publication