CN204101448U - A kind of spectrum beam splitting measurement mechanism for Supercontinuum source - Google Patents

A kind of spectrum beam splitting measurement mechanism for Supercontinuum source Download PDF

Info

Publication number
CN204101448U
CN204101448U CN201420561904.7U CN201420561904U CN204101448U CN 204101448 U CN204101448 U CN 204101448U CN 201420561904 U CN201420561904 U CN 201420561904U CN 204101448 U CN204101448 U CN 204101448U
Authority
CN
China
Prior art keywords
pass filter
wave pass
optical fiber
fiber collimator
long wave
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.)
Expired - Fee Related
Application number
CN201420561904.7U
Other languages
Chinese (zh)
Inventor
刘博文
黄昊
宋寰宇
胡明列
王清月
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.)
Tianjin University
Original Assignee
Tianjin University
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 Tianjin University filed Critical Tianjin University
Priority to CN201420561904.7U priority Critical patent/CN204101448U/en
Application granted granted Critical
Publication of CN204101448U publication Critical patent/CN204101448U/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Landscapes

  • Spectrometry And Color Measurement (AREA)

Abstract

A kind of spectrum beam splitting measurement mechanism for Supercontinuum source, use three optical fiber collimators and a long wave pass filter or short wave pass filter, the super continuum light spectrum that Supercontinuum source is exported by tail optical fiber is collimated by an optical fiber collimator, and then be incident on long wave pass filter or short wave pass filter, be divided into long wave and shortwave two parts by long wave pass filter or short wave pass filter transmission or reflection according to the cutoff wavelength of long wave pass filter or short wave pass filter, transmission or the two-way light reflected is each respectively is again coupled in determinand through an optical fiber collimator, adopt two of corresponding range spectrometers to measure the transmitted spectrum of determinand respectively more respectively simultaneously.The utility model achieves and uses grating spectrograph to carry out the seamless measurement of ultra broadband in the whole spectral range of Supercontinuum source simultaneously.Device of the present utility model does not need to regulate light path to change different narrow band pass filters before every measurement, both time saving and energy saving, reduces cost, turn increases stability and the reliability of device.

Description

A kind of spectrum beam splitting measurement mechanism for Supercontinuum source
Technical field
The utility model relates to a kind of spectrum beam splitting measuring method and device.Particularly relate to and a kind ofly utilize bulk optics device super continuum light to be composed length wave component to carry out beam splitting so that carry out the spectrum beam splitting measurement mechanism for Supercontinuum source measured in whole spectral range simultaneously.
Background technology
The transmitting procedure of light pulse in nonlinear medium, not only be subject to the impact of the multiple nonlinear effects such as such as Self-phase modulation (SPM), Cross-phase Modulation (XPM), four-wave mixing (FWM), stimulated Raman scattering (SRS) and stimulated Brillouin scattering (SBS), be also subject to the impact of Dispersion of Media characteristic.Under the acting in conjunction of nonlinear effect and dispersion, new frequency component is produced.For enough strong pulse, its spectrum can be more than broadened hundreds of nanometer, and this phenomenon is referred to as the generation of super continuum light spectrum.
Supercontinuum source can export ultra-wide spectrum laser, and it to have on the field of high request low-coherence light source or spectral analysis in biology, medical science, physics, national defence and industry etc. and has important application.In spectroscopy applications, because Supercontinuum source can export the pole wide spectral more than an even several octave, thus a Supercontinuum source just can substitute before the narrow-band light source of several different-waveband, enormously simplify the complexity of system source.
But from the viewpoint of spectral measurement, the equipment that present stage mainly uses is grating spectrograph.Relative to the spectral bandwidth of Supercontinuum source, the range of grating spectrograph is very limited, about being generally an octave, such as: the range of two kinds of conventional grating spectrographs is respectively 600-1700nm and 1200-2400nm.Particularly close to 2 micron wavebands of middle infrared, market almost only have range be that this kind of spectrometer of 1200-2400nm is available.
According to grating equation known, rudimentary diffraction of long wavelength light signal overlaps completely by corresponding senior diffraction of short-wavelength light signal, cannot separate.Such as: wavelength is that the light of 2100nm enters to inject in grating spectrograph, its first-order diffraction can be the second-order diffraction of 1050nm light with wavelength, wavelength be 700nm light three order diffractions and by that analogy more senior the diffraction light of short wavelength overlap completely.Even if the light that its consequence is in fact not 2100nm enters spectrometer and only has the above-mentioned short-wavelength light mentioned to enter into spectrometer, spectrometer also can show and recorded the light signal that wavelength is 2100nm, thus causes measuring error.
Further, existing Supercontinuum source uses the Yb dosed optical fiber mode-locked laser being operated in 1 micron waveband as seed light source mostly, and after amplifying, pumped nonlinear optical fiber produces super continuum light spectrum.The light intensity of the shortwave part that this makes super continuum light compose especially 1 micron waveband is better than long wavelength part.In addition the shortwave part of super continuum light spectrum has been significantly shorter than the short-wavelength limit 1200nm of spectrometer range.Final result is that the long wavelength part of measurement result, especially at 2 micron wavebands, above-mentioned measuring error has been typically further exacerbated under the outrange of 1 stronger micron waveband light signal and spectrometer to use both acting in conjunction.
At present, when applying Supercontinuum source and carrying out spectroscopy applications, the main method solved the problem adopts corresponding narrow band pass filter to leach corresponding spectral component according to the wave band of application.But the inferior position of this method is also apparent.On the one hand, the spectral component be in narrow band pass filter rejection zone will be lost completely, can not apply.This is the significant wastage spectral width of Supercontinuum source not only, also weakens its advantage compared with traditional narrow light source.On the other hand, in order to meet the demand of ultra-wideband detection, such scheme must need several narrow band pass filter, not only increases the cost of device, and each narrow band pass filter of changing all needs to readjust light path, wastes time and energy.
Such as: in the application utilizing Supercontinuum source measuring optical fiber grating, if two fiber gratings having centre wavelength to be respectively 1.5 microns and 2 microns need to measure.Two narrow band pass filters needing reserve centre wavelength to be respectively 1.5 microns and 2 microns according to above-mentioned solution are measured at twice, and each measure before all need to readjust light path.
Summary of the invention
Technical problem to be solved in the utility model is, there is provided a kind of whole wave band of Supercontinuum source that can make full use of to measure in real time, do not need to regulate light path to change different narrow band pass filters before every measurement, and the stability of device and the spectrum beam splitting measurement mechanism for Supercontinuum source of reliability can be increased.
The technical scheme that the utility model adopts is: a kind of spectrum beam splitting measurement mechanism for Supercontinuum source, include the first optical fiber collimator, second optical fiber collimator, 3rd optical fiber collimator and long wave pass filter or short wave pass filter, the light incident side of the first described optical fiber collimator is by Fiber connection Supercontinuum source, described long wave pass filter or short wave pass filter are arranged on the output light path of described first optical fiber collimator, described second optical fiber collimator is arranged on the reflected light path of described long wave pass filter or short wave pass filter, described 3rd optical fiber collimator is arranged on the transmitted light path of described long wave pass filter or short wave pass filter, the light output end of the second described optical fiber collimator connects the first determinand, the light output end of the 3rd described optical fiber collimator connects the second determinand, the light output end of described first determinand connects the first spectrometer, the light output end of described second determinand connects the second spectrometer.
The cutoff wavelength of described long wave pass filter or short wave pass filter is greater than the range short-wavelength limit for the second spectrometer or the first spectrometer of measuring long wavelength part spectrum when using long wave pass filter or short wave pass filter respectively.
A kind of spectrum beam splitting measurement mechanism for Supercontinuum source of the present utility model, not only takes full advantage of the whole spectral bandwidth of Supercontinuum source, makes the spectrum simultaneously measuring different-waveband determinand become possibility; Achieve and use grating spectrograph to carry out the seamless measurement of ultra broadband in the whole spectral range of Supercontinuum source simultaneously.Device of the present utility model is used also not need to regulate light path to change different narrow band pass filters before every measurement, both time saving and energy saving, reduce cost, turn increase stability and the reliability of device.
Accompanying drawing explanation
Fig. 1 is one-piece construction schematic diagram of the present utility model;
Fig. 2 is the result that the first testing fiber grating measuring of the first spectrometer to 1.5 micron wavebands obtains;
Fig. 3 is the result that the second testing fiber grating measuring of the second spectrometer to 2 micron wavebands obtains.
In figure
1: the first optical fiber collimator 2: the second optical fiber collimator
3: the three optical fiber collimators 4: long wave pass filter or short wave pass filter
5: the first determinand 6: the second determinands
7: the first spectrometer 8: the second spectrometers
9: Supercontinuum source 10: optical fiber
Embodiment
Below in conjunction with embodiment and accompanying drawing, a kind of spectrum beam splitting measurement mechanism for Supercontinuum source of the present utility model is described in detail.
A kind of spectrum beam splitting measurement mechanism for Supercontinuum source of the present utility model, be divided into length ripple two parts to apply respectively super continuum light spectrum by bulk optics device, can be implemented in the whole spectral range of Supercontinuum source and use grating spectrograph to carry out this target of the seamless measurement of ultra broadband simultaneously.
As shown in Figure 1, a kind of spectrum beam splitting measurement mechanism for Supercontinuum source of the present utility model, include the first optical fiber collimator 1, second optical fiber collimator 2, 3rd optical fiber collimator 3 and long wave pass filter or short wave pass filter 4, the light incident side of the first described optical fiber collimator 1 connects Supercontinuum source 9 by optical fiber 10, described long wave pass filter or short wave pass filter 4 are arranged on the output light path of described first optical fiber collimator 1, and, the output light path of described long wave pass filter or short wave pass filter 4 and the first described optical fiber collimator 1, and the output light path of the reflected light path of long wave pass filter or short wave pass filter 4 and the first described optical fiber collimator 1 to need and filbtercharacteristic can arrange and has a certain degree according to measuring, as the output light path of the first optical fiber collimator with the incident angles of 20 degree on long wave pass filter or short wave pass filter 4, namely the reflected light path of long wave pass filter or short wave pass filter 4 and the output light path of the first described optical fiber collimator 1 are 40 degree of angles.
Described second optical fiber collimator 2 is arranged on the reflected light path of described long wave pass filter or short wave pass filter 4, described 3rd optical fiber collimator 3 is arranged on the transmitted light path of described long wave pass filter or short wave pass filter 4, the light output end of the second described optical fiber collimator 2 connects the first determinand 5, the light output end of the 3rd described optical fiber collimator 3 connects the second determinand 6, the light output end of described first determinand 5 connects the first spectrometer 7, and the light output end of described second determinand 6 connects the second spectrometer 8.The cutoff wavelength of described long wave pass filter or short wave pass filter 4 is greater than the range short-wavelength limit for the second spectrometer 8 or the first spectrometer 7 of measuring long wavelength part spectrum when using long wave pass filter or short wave pass filter 4 respectively.
The Supercontinuum source output spectrum bandwidth that the utility model uses in a particular embodiment is 800-2100nm, collimated light is become through the first reflective optical fiber collimator after super continuum light spectrum is exported by tail optical fiber, and with the incident angles of 20 degree on long wave pass filter.The cutoff wavelength of long wave pass filter is 1700nm, is greater than the short-wavelength limit 1200nm measuring long wavelength part grating spectrograph range used.Like this, the ultra-wide spectrum that Supercontinuum source exports will be that boundary is divided into two bundles with 1700nm, and the part of 800-1700nm will be reflected onto in the second optical fiber collimator, and the part of 1700-2100nm will be transmitted through in the 3rd optical fiber collimator.Two-beam is coupled in optical fiber by the second optical fiber collimator and the 3rd optical fiber collimator respectively, transfers to the first determinand and the second determinand.Finally, measure the transmitted spectrum of the first determinand and the second determinand with two spectrometers that range is 600-1700nm and 1200-2400nm respectively simultaneously, result as shown in Figures 2 and 3 can be obtained respectively.First determinand and the second determinand are respectively the fiber grating of 1.5 microns and 2 micron wavebands, can read the parameters such as centre wavelength, reflectivity and the bandwidth of the two from figure.The first determinand wherein and the second determinand can be the printing opacity objects such as fiber grating, bulk crystals, biological tissue's thin slice.
It will be appreciated by those skilled in the art that accompanying drawing is the schematic diagram of a preferred embodiment, above-mentioned the utility model embodiment sequence number, just to describing, does not represent the quality of embodiment.
The foregoing is only preferred embodiment of the present utility model, not in order to limit the utility model, all within spirit of the present utility model and principle, any amendment done, equivalent replacement, improvement etc., all should be included within protection domain of the present utility model.

Claims (2)

1. the spectrum beam splitting measurement mechanism for Supercontinuum source, include the first optical fiber collimator (1), second optical fiber collimator (2), 3rd optical fiber collimator (3) and long wave pass filter or short wave pass filter (4), it is characterized in that, the light incident side of described the first optical fiber collimator (1) connects Supercontinuum source (9) by optical fiber (10), described long wave pass filter or short wave pass filter (4) are arranged on the output light path of described first optical fiber collimator (1), described second optical fiber collimator (2) is arranged on the reflected light path of described long wave pass filter or short wave pass filter (4), described 3rd optical fiber collimator (3) is arranged on the transmitted light path of described long wave pass filter or short wave pass filter (4), the light output end of described the second optical fiber collimator (2) connects the first determinand (5), the light output end of the 3rd described optical fiber collimator (3) connects the second determinand (6), the light output end of described first determinand (5) connects the first spectrometer (7), the light output end of described second determinand (6) connects the second spectrometer (8).
2. a kind of spectrum beam splitting measurement mechanism for Supercontinuum source according to claim 1, it is characterized in that, the cutoff wavelength of described long wave pass filter or short wave pass filter (4) is greater than the range short-wavelength limit for the second spectrometer (8) or the first spectrometer (7) of measuring long wavelength part spectrum when using long wave pass filter or short wave pass filter (4) respectively.
CN201420561904.7U 2014-09-26 2014-09-26 A kind of spectrum beam splitting measurement mechanism for Supercontinuum source Expired - Fee Related CN204101448U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201420561904.7U CN204101448U (en) 2014-09-26 2014-09-26 A kind of spectrum beam splitting measurement mechanism for Supercontinuum source

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201420561904.7U CN204101448U (en) 2014-09-26 2014-09-26 A kind of spectrum beam splitting measurement mechanism for Supercontinuum source

Publications (1)

Publication Number Publication Date
CN204101448U true CN204101448U (en) 2015-01-14

Family

ID=52269867

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201420561904.7U Expired - Fee Related CN204101448U (en) 2014-09-26 2014-09-26 A kind of spectrum beam splitting measurement mechanism for Supercontinuum source

Country Status (1)

Country Link
CN (1) CN204101448U (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104237141A (en) * 2014-09-26 2014-12-24 天津大学 Spectral splitting measurement method and device for supercontinuum source

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104237141A (en) * 2014-09-26 2014-12-24 天津大学 Spectral splitting measurement method and device for supercontinuum source

Similar Documents

Publication Publication Date Title
CN103219638B (en) A kind of super continuum source and coherent anti-stokes raman scattering imaging system
Paterova et al. Measurement of infrared optical constants with visible photons
US11300452B2 (en) Spectral measurement method, spectral measurement system, and broadband pulsed light source unit
CN110832295B (en) Real-time optical spectrum-time analyzer and method
CN102313605B (en) Method and device for measuring self-referenced spectral interference femtosecond laser pulse in real time
EP2522969A2 (en) Nonlinear raman spectroscopic apparatus comprising single mode fiber for generating Stokes beam
Butler et al. Multi-octave spanning, Watt-level ultrafast mid-infrared source
CN104236725B (en) A kind of device and method of accurate measurement optical maser wavelength
Tzankov et al. Broadband optical parametric amplification in the near UV–VIS
CN106092337A (en) The calibrating installation of a kind of ultraviolet wavelength measuring instrument and method
Pawłowska et al. Shaping and spatiotemporal characterization of sub-10-fs pulses focused by a high-NA objective
US9195042B2 (en) Laser based apparatus, methods and applications
CN107505055A (en) Minimize linear pattern femto-second laser pulse shape width of measuring device
Dimitrov et al. Pulse front tilt measurement of femtosecond laser pulses
Ding et al. A fast interrogation system of FBG sensors based on low loss jammed-array wideband sawtooth filter
CN204101448U (en) A kind of spectrum beam splitting measurement mechanism for Supercontinuum source
WO2020196692A1 (en) Broadband pulse light source device, spectrometry device, and spectrometry method
CN104237141B (en) A kind of spectrum beam splitting measuring method for Supercontinuum source and device
CN104237141A (en) Spectral splitting measurement method and device for supercontinuum source
Zhu et al. Self-calibrating fiber spectrometer for the measurement of broadband downconverted photon pairs
CN103604509A (en) Device and method for measuring ultra-short pulse laser residual angular dispersion
DE102007042172A1 (en) Low optical losses e.g. transmission losses, measurement method for determining of e.g. absorption spectrum of gases, involves utilizing sequential signal recording by software-controlled signal processing electronic system
CN102778301A (en) Real-time measuring device of self-reference spectrum interference femtosecond laser pulse
CN104913847A (en) Device and method for measuring high-intensity terahertz time-domain spectroscopy
US20130265581A1 (en) System and Method for Measuring Phase-Matching Spectral Phase Curve by Nonlinear Optical Spectral Interferometry

Legal Events

Date Code Title Description
C14 Grant of patent or utility model
GR01 Patent grant
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20150114

Termination date: 20150926

EXPY Termination of patent right or utility model