CN104515742B - Method for improving cavity ring-down time measurement accuracy - Google Patents
Method for improving cavity ring-down time measurement accuracy Download PDFInfo
- Publication number
- CN104515742B CN104515742B CN201410789135.0A CN201410789135A CN104515742B CN 104515742 B CN104515742 B CN 104515742B CN 201410789135 A CN201410789135 A CN 201410789135A CN 104515742 B CN104515742 B CN 104515742B
- Authority
- CN
- China
- Prior art keywords
- cavity
- down time
- threshold value
- ring
- gas
- 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
Links
Landscapes
- Investigating Or Analysing Materials By Optical Means (AREA)
Abstract
The invention relates to a method for improving cavity ring-down time measurement accuracy. The method comprises the following steps: starting a laser and locking the wavelength within the range of characteristic spectrum lines of the gas to be tested according to a wavelength looped system; adjusting the length of a resonant cavity while monitoring the amplitude of signals output by a detector; stopping adjusting the length of the resonant cavity until the amplitude of the signals output by the detector reaches a set upper threshold value, and then shutting down the laser; starting timing when the amplitude of the signals output by the detector reaches the set upper threshold value again; stopping timing when the amplitude of the signals output by the detector reaches a set lower threshold value; calculating the free ring-down time constant of the cavity; pumping the gas to be tested into the cavity and repeating the previous steps to obtain the free ring-down time constant of the cavity containing the gas to be tested; calculating the concentration of the gas in the cavity according to data such as the free ring-down time constant of the cavity and that of the cavity containing the gas to be tested. According to the invention, the semiconductor laser is quickly shut down through electric current, which reduces the impact of the tailing on the measurement data.
Description
Technical field
The present invention relates to trace gas detects picosecond time interval measurement field, particularly to a kind of improve cavity decline swing when
Between certainty of measurement method.
Background technology
Cavity ring-down spectroscopy technology (crds, cavity ring-down spectrum) it is that a kind of recent two decades develop
The trace gas Detection Techniques come, the resonator that its core technology is made up of ultra-high reflectivity speculum, narrow linewidth laser
And wavelength locking technology and precise time-time-interval e measurement technology.In terms of measurement trace gas, the isotopic content of trace element
There are very many advantages, such as measurement data is unrelated with laser power fluctuation, do not need standard sample gas, certainty of measurement pole
High, can complete to measure in real time, need not calibrate for a long time, field unattended measurement etc..
Due to cavity ring-down spectroscopy commercial measurement high precision, specular reflectivity and time resolution are required also very
High.As shown in subordinate list one, in the long 41cm in chamber, specular reflectivity is 0.9999, and linear function is under 5.13 and room temperature normal pressure, divide
Distinguish 30ppbv methane gas content when, time resolution be 4.5ns;And when gas concentration resolution ratio is 1ppbv, the time
Certainty of measurement is 0.15ns.On the premise of in chamber, specular reflectivity can not improve, time resolution brings up to from 4.5ns
0.15ns, this proposes high requirement to time measurement system.The present invention is exactly directed to this situation, from ring-down time starting point
Be accurately positioned to improve the precision of time measurement with two aspects of accurate measurement at ring-down time interval.
Content of the invention
The invention solves the problems that technical problem of the prior art, provide a kind of side improving cavity ring-down time certainty of measurement
Method.
In order to solve above-mentioned technical problem, technical scheme is specific as follows:
A kind of method improving cavity ring-down time certainty of measurement, comprises the following steps:
Step one, unlatching laser instrument, and by wavelength feedback regulating system, the feature of wavelength locking under test gas is inhaled
Receive in the range of spectral line;
Step 2, adjustment cavity length, and monitoring detector amplitude output signal;
Step 3, repeat step two, until detector output signal amplitude reaches the upper threshold value of setting, stop adjustment chamber
Long, and close laser instrument;
Step 4, resonator no longer have energy input, and freedom of entry declines the stage of swinging, and energy is gradually decayed, when detector is defeated
When going out signal amplitude again for setting upper threshold value, timing starts;
Step 5, freely declining to swing proceeds, and energy is decayed further, when detector output signal amplitude reaches under setting
During threshold value, timer expiration swings end it is believed that declining;
Step 6, calculating cavity free ring-down time constant;
Step 7, suction under test gas, repeat step one to six, obtain the free ring-down time containing under test gas normal
Number;
Step 8, according to data such as the cavity that records and the free ring-down time constants containing under test gas, calculate in chamber
Gas concentration.
The present invention has a following beneficial effect:
The method of the raising cavity ring-down time certainty of measurement of the present invention, rapidly switches off semiconductor laser using electric current,
Alleviate the impact to measurement data for the conditions of streaking.
The method of the raising cavity ring-down time certainty of measurement of the present invention, accurately sets upper lower threshold value by high accuracy dac,
Reduce adc continuous sampling and judge that caused measure error, it is often more important that setting by dual threshold, eliminates closing laser
The impact to measurement for the light energy input during device.
Brief description
With reference to the accompanying drawings and detailed description the present invention is described in further detail.
Fig. 1 is System Working Principle schematic diagram.
Fig. 2 declines for light intensity in chamber and swings curve synoptic diagram.
Specific embodiment
The invention thought of the present invention is: during time of measuring interval, has several factors to lead to the decline of certainty of measurement, wherein
It is important that the positioning precision of initial time.The present invention exactly be directed to this problem, in terms of two improve to initial when
The positioning precision carved, and then improve the certainty of measurement of time interval in the measurement of cavity ring-down spectroscopy.
Specifically, the method for the raising cavity ring-down time certainty of measurement of the present invention, comprises the following steps:
Open laser instrument, and by wavelength feedback regulating system by the characteristic absorpting spectruming line model of wavelength locking under test gas
In enclosing;
Adjustment cavity length, and monitoring detector amplitude output signal, set until detector output signal amplitude reaches
Fixed upper threshold value, stopping adjustment chamber is long, and closes laser instrument;
When detector output signal amplitude is to set upper threshold value again, timing starts;
When detector output signal amplitude reaches setting lower threshold value, timer expiration;
Calculate cavity free ring-down time constant;
Suction under test gas, repeat the above steps, obtain the free ring-down time constant containing under test gas;
According to the data such as the cavity recording and the free ring-down time constant containing under test gas, calculate intracavity gas dense
Degree.
Below in conjunction with the accompanying drawings 1 and accompanying drawing 2 illustrate the present invention step realize.
A kind of method improving cavity ring-down time certainty of measurement, comprises the following steps:
Step one, device power-on, open laser instrument 2, and controller 101 passes through temperature-driven 102 and electric current drives 103 regulations
The wavelength of laser instrument 2, and monitor wavelength change with Wavelength monitor (in figure does not provide), and wavelength locking is inhaled in gas characteristic
Receive in the range of spectral line;
Step 2, transit chamber long adjustment unit (in figure is not given) adjust the length of resonator 3, and are monitored with detector 4
Resonator 3 output intensity;
Step 3, repeat step two, until the signal amplitude of detector 4 output reaches the upper threshold value v1 of setting (in accompanying drawing 2
The t1 moment), stop adjustment chamber long, and by electric current drive 103 close laser instruments 2;
Step 4, resonator 3 no longer have energy input, and freedom of entry declines the stage of swinging, and energy is gradually decayed, when detector 4
Amplitude output signal is to set upper threshold value v1 (the t2 moment in accompanying drawing 2) again, and timing starts;
Step 5, freely declining to swing proceeds, and energy is decayed further, when detector 4 amplitude output signal reaches setting
During lower threshold value v2 (t3 moment in accompanying drawing 2), timing stops swinging end it is believed that declining;
Step 6, comparator 5 and time measurement module 6, by the time interval length between t2 to t3, calculate cavity freely
Ring-down time constant;
Step 7, suction under test gas, repeat step one to six, obtain the free ring-down time containing under test gas normal
Number;
Step 8, according to data such as the cavity that records and the free ring-down time constants containing under test gas, calculate in chamber
Gas concentration.
Cavity ring-down spectroscopy measurement process is as follows:
First turn on laser instrument, by regulating system, laser wavelength is adjusted in the characteristic absorpting spectruming line of gas, so
Wavelength locking afterwards, adjusts cavity length, when light beam makes energy close laser instrument when increasing to setting upper threshold value in chamber interior resonance,
At this moment no longer there is energy input in chamber, enter and decline the stage of swinging, until intra-cavity energy decays to setting lower threshold value, decline and swing process knot
Bundle.Decay to time interval between lower threshold value by measuring energy from upper threshold value, ring-down time constant can be calculated, thus
Calculate the concentration of under test gas in chamber.Can be seen that from the above-mentioned course of work at 2 points: one, when intra-cavity energy runs up to setting upper-level threshold
During value, the closing velocity of laser instrument will affect the positioning precision of initial time;2nd, ring-down time is spaced longer, then time measurement
The impact to certainty of measurement for module itself measure error is less.
Used in cavity ring-down spectroscopy, laser instrument is semiconductor laser, can pass through temperature and two kinds of driving current
Mode adjusts laser wavelength, because rate temperature change is relatively slowly a lot, by the way of adjustment electric current, by laser instrument ripple
Long rapid removal characteristic absorpting spectruming line scope, is equivalent to and closes laser instrument, the perseverance that additional drive circuit produces for parallel dac
Stream source, this process just can complete in 30ns.Even the so short time, cavity ring-down spectroscopy e measurement technology is come
Say still difficult to accept, can be confirmed by table 1.If reaching the moment of upper threshold value as initial time from intra-cavity energy,
In laser instrument closing process, intra-cavity energy still increases quick, therefore after intra-cavity energy reaches upper threshold value, closes laser
Device, when intra-cavity energy is re-lowered to upper threshold value, timing starts, and sees accompanying drawing 2.It is upper by high-precision dac output voltage
Lower threshold value comparative level, ultrahigh-speed comparator producing ratio relatively exports, when at this moment can accurately provide declining between lower threshold value and swinging
Between length.
Relation table between table 1. time of measuring precision and gas concentration
Data above design conditions are: the long 41cm in chamber, and cavity mirrors reflectivity is 0.9999, standard atmospheric pressure, room temperature (25 DEG C),
Linear function is 5.13.
Obviously, above-described embodiment is only intended to clearly illustrate example, and the not restriction to embodiment.Right
For those of ordinary skill in the art, can also make on the basis of the above description other multi-forms change or
Change.There is no need to be exhaustive to all of embodiment.And the obvious change thus extended out or
Change among still in the protection domain of the invention.
Claims (3)
1. a kind of method improving cavity ring-down time certainty of measurement is it is characterised in that comprise the following steps:
Step one, open laser instrument, and by wavelength feedback regulating system by the characteristic absorpting spectrum of wavelength locking under test gas
In the range of line;
Step 2, adjustment cavity length, and monitoring detector amplitude output signal;
Step 3, repeat step two, until detector output signal amplitude reaches the upper threshold value of setting, stopping adjustment chamber is long, and
Close laser instrument;
Step 4, resonator no longer have energy input, and freedom of entry declines the stage of swinging, and energy is gradually decayed, when detector exports letter
When number amplitude is to set upper threshold value again, timing starts;
Step 5, freely declining to swing proceeds, and energy is decayed further, when detector output signal amplitude reaches setting lower threshold value
When, timer expiration swings end it is believed that declining;
Step 6, calculating cavity free ring-down time constant.
2. the method improving cavity ring-down time certainty of measurement as claimed in claim 1 is it is characterised in that after step 6
Also include:
Step 7, suction under test gas, repeat step one to six, obtain the free ring-down time constant containing under test gas.
3. the method improving cavity ring-down time certainty of measurement as claimed in claim 2 is it is characterised in that after step 7
Also include:
Cavity and the free ring-down time constant data containing under test gas that step 8, basis record, calculate intracavity gas dense
Degree.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201410789135.0A CN104515742B (en) | 2014-12-17 | 2014-12-17 | Method for improving cavity ring-down time measurement accuracy |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201410789135.0A CN104515742B (en) | 2014-12-17 | 2014-12-17 | Method for improving cavity ring-down time measurement accuracy |
Publications (2)
Publication Number | Publication Date |
---|---|
CN104515742A CN104515742A (en) | 2015-04-15 |
CN104515742B true CN104515742B (en) | 2017-01-18 |
Family
ID=52791369
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201410789135.0A Expired - Fee Related CN104515742B (en) | 2014-12-17 | 2014-12-17 | Method for improving cavity ring-down time measurement accuracy |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN104515742B (en) |
Families Citing this family (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN107389604B (en) * | 2017-06-26 | 2019-08-20 | 中国科学院光电研究院 | A kind of laser, which declines, swings detection method |
CN107561009A (en) * | 2017-09-12 | 2018-01-09 | 中国科学院长春光学精密机械与物理研究所 | Resonator output intensity determines method, system and measuring apparatus, concentrations detectors |
CN109959623B (en) * | 2017-12-25 | 2024-08-27 | 内蒙古光能科技有限公司 | Sampling system and sampling method of CRDS gas concentration detector |
CN114166766B (en) * | 2021-12-06 | 2024-05-14 | 中国科学院合肥物质科学研究院 | Gas measurement method based on amplitude modulation cavity enhanced absorption spectrum technology |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN103471815A (en) * | 2013-09-11 | 2013-12-25 | 中国科学院光电技术研究所 | Method for simultaneously measuring reflectivity of S and P polarized light of high-reflection mirror |
CN203745374U (en) * | 2013-11-12 | 2014-07-30 | 西安泰戈瑞森仪器有限公司 | Cavity ring-down-based online trace gas analysis device |
Family Cites Families (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US8325343B2 (en) * | 2010-02-16 | 2012-12-04 | Honeywell International Inc. | Detector for cavity ring-down spectroscopy |
JP2014516405A (en) * | 2011-03-25 | 2014-07-10 | ユニバーシティ オブ ヴァージニア パテント ファウンデーション | Cell design compatible with spectrometer |
US8681827B2 (en) * | 2011-05-16 | 2014-03-25 | Oewaves, Inc. | Generation of single optical tone, RF oscillation signal and optical comb in a triple-oscillator device based on nonlinear optical resonator |
-
2014
- 2014-12-17 CN CN201410789135.0A patent/CN104515742B/en not_active Expired - Fee Related
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN103471815A (en) * | 2013-09-11 | 2013-12-25 | 中国科学院光电技术研究所 | Method for simultaneously measuring reflectivity of S and P polarized light of high-reflection mirror |
CN203745374U (en) * | 2013-11-12 | 2014-07-30 | 西安泰戈瑞森仪器有限公司 | Cavity ring-down-based online trace gas analysis device |
Non-Patent Citations (4)
Title |
---|
Cavity Enhanced Spectroscopy: Applications Theory and Instrumentation;Cora J. Young et al.;《Encyclopedia of Analytical Chemistry》;20111231;1-20 * |
Cavity ring-down spectroscopy;Martyn D. Wheeler et al.;《Journal of the Chemical Society, Faraday Transactions》;19980101;第94卷(第3期);337-351 * |
光腔衰荡高反射率测量技术综述;李斌成,龚元;《激光与光电子学进展》;20101231;第47卷;021203-1至021203-11 * |
腔衰荡光谱技术中衰荡时间的准确快速提取;王丹等;《光谱学与光谱分析》;20141031;第34卷(第10期);2845-2850 * |
Also Published As
Publication number | Publication date |
---|---|
CN104515742A (en) | 2015-04-15 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN104515742B (en) | Method for improving cavity ring-down time measurement accuracy | |
Jiang et al. | TDLAS-based detection of dissolved methane in power transformer oil and field application | |
US7351954B2 (en) | Method and apparatus for detecting gas concentration with infrared absorption characteristics | |
JP6981817B2 (en) | Spectroscopic analyzer and spectroscopic analysis method | |
CN102735643B (en) | Device and method for measuring water vapor content by using self-calibrating optical cavity ring-down spectroscopy | |
CN108181266B (en) | TD L AS gas concentration detection method | |
US9207169B2 (en) | Laser spectrometer and method for measuring concentration of a gas component in a measurement gas | |
CN108956544B (en) | Automatic detection system and method for transverse relaxation time of atoms | |
CN203148832U (en) | Double-channel cavity-ring-down atmospheric aerosol extinction instrument | |
CN106500911B (en) | Pressure gauge calibration method based on gas absorption spectral line pressure broadening effect | |
JP2015531071A (en) | External cavity laser absorption spectroscopy method and apparatus | |
CN106017783A (en) | Method of measuring pressures of two gases in alkali metal gas chamber simultaneously | |
CN110940422B (en) | MEMS infrared detector response time measuring device and method | |
CN110045309B (en) | Novel optical pump magnetometer precision self-detection method | |
EP2549265A1 (en) | Laser gas analysis apparatus | |
JP4633103B2 (en) | Optical frequency measurement method and apparatus | |
TW201314194A (en) | Object characteristics measurement system | |
US11879833B2 (en) | Circular dichroism measurement device and circular dichroism measurement method | |
JP5258294B2 (en) | Method for improving optical measurement of gas concentration | |
CN104316887A (en) | Performance test method and device for laser xenon lamp | |
US11796468B2 (en) | Gas measurement device and gas measurement method | |
CN105866068A (en) | Recursive least squares technology-based laser absorption spectrum harmonic signal peak point extraction method | |
CN108426850A (en) | CO in a kind of absolute measurement air2The frequency stabilization cavity ring-down spectroscopy instrument of content | |
CN108398393A (en) | A kind of the cavity ring-down spectroscopy instrument and measurement method of quick measurement greenhouse gases content | |
CN107884364A (en) | Temperature and humidity compensation method when being detected available for laser methane |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
C06 | Publication | ||
PB01 | Publication | ||
C10 | Entry into substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
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: 20170118 Termination date: 20211217 |
|
CF01 | Termination of patent right due to non-payment of annual fee |