CN104697933B - Triple channel acoustic resonant cavity optoacoustic spectroscopy sensing device - Google Patents

Triple channel acoustic resonant cavity optoacoustic spectroscopy sensing device Download PDF

Info

Publication number
CN104697933B
CN104697933B CN201510096806.XA CN201510096806A CN104697933B CN 104697933 B CN104697933 B CN 104697933B CN 201510096806 A CN201510096806 A CN 201510096806A CN 104697933 B CN104697933 B CN 104697933B
Authority
CN
China
Prior art keywords
acoustic
resonator
resonant cavity
laser
conducting pipe
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.)
Active
Application number
CN201510096806.XA
Other languages
Chinese (zh)
Other versions
CN104697933A (en
Inventor
刘锟
谈图
汪磊
王贵师
朱公栋
梅教旭
高晓明
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.)
Hefei Institutes of Physical Science of CAS
Original Assignee
Hefei Institutes of Physical Science of CAS
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 Hefei Institutes of Physical Science of CAS filed Critical Hefei Institutes of Physical Science of CAS
Priority to CN201510096806.XA priority Critical patent/CN104697933B/en
Publication of CN104697933A publication Critical patent/CN104697933A/en
Application granted granted Critical
Publication of CN104697933B publication Critical patent/CN104697933B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Abstract

The invention discloses a kind of triple channel acoustic resonant cavity optoacoustic spectroscopy sensing device.It includes the laser controller (2) and the control signal source that are electrically connected with laser successively, and the tubulose acoustic resonant cavity that is communicated with acoustic conducting pipe coaxial with laser light path, it is placed in the acoustic sensor (5) of its output end electrical connection lock-in amplifier (6) of acoustic conductance pipe port, particularly laser, laser controller (2) and it is three as the signal generator (1) in control signal source, tubulose acoustic resonant cavity is by cylinder (7), its tubulose cavity axis is constituted with three resonators of cylinder (7) diameter parallel, the pipe port of three acoustic conducting pipes is respectively positioned on the sensitive face of acoustic sensor (5), three signal output parts of three passage tapped off signal generator (1) of lock-in amplifier (6), the three road photoacoustic spectrum signals for going out acoustic sensor (5) perception by demodulation reference signal.Three kinds of components in its energy synchronous real-time measurement gas.

Description

Triple channel acoustic resonant cavity optoacoustic spectroscopy sensing device
Technical field
The present invention relates to a kind of optoacoustic spectroscopy sensing device, especially a kind of triple channel acoustic resonant cavity optoacoustic spectroscopy sensing Device.
Background technology
Optoacoustic spectroscopy is a kind of spectral technique based on optoacoustic effect, detection be the light energy that is absorbed by the sample rather than Transmitted light intensity.When the light source in molecule absorption wave band is irradiated on sample, sample molecule absorbs light energy and transits to sharp Hair state, the molecule in excitation state returns to ground state by collision relaxation, while the light energy for absorbing is converted into the interior energy of molecule, and The local temperature of molecule is caused to raise.So when the light being irradiated on sample molecule is modulated, the local temperature of molecule is just Periodically change can be produced, so as to produce periodic pressure change, i.e. sound wave.When with acoustic sensor record acoustical signal with During the variation relation of optical source wavelength, photoacoustic spectrum signals have just been obtained.Due to optoacoustic spectroscopy photoacoustic signal only with material to light Absorption it is relevant, do not influenceed by the scattering factor such as light, therefore be well suited for for the detection to material optical absorption characteristics, such as China A kind of optoacoustic spectroscopy gas sensor that patent of invention CN 102954948B were announced on November 12nd, 2014.The patent of invention Using the T-shaped acoustic resonance cavity being made up of supervisor and branch pipe vertical connection, and make the pipe axis of supervisor coaxial with light source optical path, light path On the focus of condenser lens be located at supervisor and the connectivity part of branch pipe, as the quartz tuning-fork of sonic transducer prong plane and Slit center respectively with the axis perpendicular of branch pipe and the structure on axis;During detection, by T-shaped acoustic resonance cavity to optoacoustic The acoustic resonance of signal amplifies, and detects and determine the content of trace gas.Though it can in maximum efficiency realize that light excites sound wave Coupling between energy and quartz tuning-fork, for detection trace gas field, be but difficult to multi-wavelength under test gas, Multi-component synchronous real-time measurement.In reality, realized to different component in gas using same optoacoustic spectroscopy gas sensor The demand of synchronous real-time measurement be objective reality, such as in the research of aerosol absorption characteristic, just need to be to the suction of aerosol Receiving characteristic carries out multi-wavelength synchro measure, and then analyzes the wavelength-dependent behavior of its absorption, aerosol absorptionSystem Number etc..
The content of the invention
The technical problem to be solved in the present invention is to overcome shortcoming part of the prior art, there is provided one kind can be surveyed synchronously in real time The triple channel acoustic resonant cavity optoacoustic spectroscopy sensing device of various ingredients in amount gas.
Be to solve technical problem of the invention, the technical scheme for being used for:Triple channel acoustic resonant cavity optoacoustic spectroscopy is passed Induction device includes the laser controller and the control signal source that are electrically connected with laser successively, and the company coaxial with laser light path The tubulose acoustic resonant cavity that is connected with acoustic conducting pipe, the acoustic sensor for being placed in acoustic conductance pipe port and acoustic sensor output end are electrically connected The lock-in amplifier for connecing, particularly,
The laser is first laser device, second laser and the 3rd laser, its input tap laser controller The first control output end, the second control output end and the 3rd control output end;
The control signal source is signal generator, its first signal output part, secondary signal output end and the 3rd signal Output end taps the respective input of laser controller;
The tubulose acoustic resonant cavity is humorous by cylinder, its tubulose cavity axis parallel with cylinder axis first Shake chamber, the second resonator and the 3rd resonator composition, wherein, the first cavity length L1, the second cavity length L2 and the 3rd Relation between cavity length L3 is L1<L3<L2, the radial direction angle between the first resonator, the 3rd resonator and the second resonator It is 85~95 degree;
The acoustic conducting pipe is the first acoustic conducting pipe, the second acoustic conducting pipe and the 3rd acoustic conducting pipe, first acoustic conducting pipe, the second acoustic conductance The pipe port of pipe and the 3rd acoustic conducting pipe is respectively positioned on the sensitive face of the acoustic sensor, wherein, the first acoustic conducting pipe, the 3rd acoustic conductance The pipe axis of pipe and the angle of the sensitive face are 40~50 degree, the pipe axis of the second acoustic conducting pipe and the angle of the sensitive face It is 85~95 degree;
First letter of the first passage, second channel and the third channel tap signal generator of the lock-in amplifier Number output end, secondary signal output end and the 3rd signal output part, the reference signal for receiving signal generator offer, to solve Photoacoustic spectrum signals in the corresponding resonator of voicing sensor senses.
As the further improvement of triple channel acoustic resonant cavity optoacoustic spectroscopy sensing device:
Preferably, laser is semiconductor laser, or QCL, or optical parametric oscillation light source.
Preferably, the first cavity length L1 >=5cm, the second cavity length L2≤35cm.
Preferably, the tubular cavity diameter of the first resonator, the second resonator and the 3rd resonator is 1~15mm.
Preferably, the center of the tubulose cavity axis of the first resonator, the second resonator and the 3rd resonator is in same On circumference.
Preferably, the first acoustic conducting pipe, the second acoustic conducting pipe and the 3rd acoustic conducting pipe respectively with the first resonator, the second resonator and 3rd resonator vertical connection, and its connectivity part is respectively positioned on the midpoint of corresponding resonator.
Preferably, acoustic sensor is tuning fork, or microphone, or poly meta fluoroethylene piezoelectric film.
Preferably, the tubulose acoustic resonant cavity of cylindrical shape is disposed thereon is equipped with incidence window, exit window and enters respectively In sample mouthful, outlet, and preceding surge chamber, the photoacoustic cell of rear surge chamber.
Beneficial effect relative to prior art is:
After such structure, the present invention can it is separate, do not interfere with each other and synchronous real-time measurement three without distortion The photoacoustic signal of resonator.It realizes many ripples with just settling at one go under conditions of using only an optoacoustic spectroscopy sensing device Long, multi-component synchro measure, and each passage works in respective optimum frequency, while synchro measure is ensured, both There is provided optimal detection performance and detectivity, and the volume of measuring system and the volume of sample are greatly reduced, from And greatly extend its applicable scope.
Brief description of the drawings
Fig. 1 is a kind of basic structure schematic diagram of the invention.
Fig. 2 is triple channel acoustic resonant cavity and corresponding acoustic conducting pipe in the present invention, and the connection between acoustic sensor Connection diagram.
Fig. 3 is the distribution of lengths schematic diagram of triple channel acoustic resonant cavity in the present invention.
Fig. 4 is the frequency characteristic curve diagram of triple channel acoustic resonant cavity in the present invention.
Specific embodiment
Preferred embodiment of the invention is described in further detail below in conjunction with the accompanying drawings.
Referring to Fig. 1, Fig. 2 and Fig. 3, the composition of triple channel acoustic resonant cavity optoacoustic spectroscopy sensing device is as follows:
First laser device 301, the input of the laser 303 of second laser 302 and the 3rd are sequentially connected electrically laser respectively First control output end 201 of controller 2, the second control output end 202 and the 3rd control output end 203, and signal occur First signal output part 101 of device 1, the signal output part 103 of secondary signal output end 102 and the 3rd;Wherein, three lasers are equal It is semiconductor laser (or QCL, or optical parametric oscillation light source).
First laser device light path 311, the laser light path of second laser light path 312 and the 3rd with above three laser The 313 coaxial tubulose acoustic resonant cavities for being communicated with acoustic conducting pipe by cylinder 7, its tubulose cavity axis with the axle of cylinder 7 The first parallel resonator 401 of line, the second resonator 402 and the 3rd resonator 403 are constituted.Wherein, the length of the first resonator 401 Relation between L1, the length L2 of the second resonator 402 and the length L3 of the 3rd resonator 403 is L1<L3<L2, now chooses the first resonance The length L1 of chamber 401 is that 5cm, the length L2 of the second resonator 402 are that 35cm, the length L3 of the 3rd resonator 403 are 15cm;First resonance The tubular cavity diameter in chamber 401, the second resonator 402 and the 3rd resonator 403 is 10 (can be 1~15) mm;First resonator 401st, the center of the tubulose cavity axis of the second resonator 402 and the 3rd resonator 403 is on same circumference, the first resonator 401st, the radial direction angle between the 3rd resonator 403 and the second resonator 402 is 90 (can be 85~95) degree.
It is the first acoustic conducting pipe 441, the second acoustic conducting pipe 442 and the 3rd sound with the acoustic conducting pipe that above three resonator is respectively communicated with Conduit 443;Wherein, the first acoustic conducting pipe 441, the second acoustic conducting pipe 442 and the 3rd acoustic conducting pipe 443 respectively with the first resonator 401, Two resonators 402 and the vertical connection of the 3rd resonator 403, and its connectivity part is respectively positioned on the midpoint of corresponding resonator.First acoustic conductance The pipe port of pipe 441, the second acoustic conducting pipe 442 and the 3rd acoustic conducting pipe 443 is respectively positioned on the sensitive face of acoustic sensor 5;Wherein, One acoustic conducting pipe 441, the pipe axis of the 3rd acoustic conducting pipe 443 and the angle of sensitive face are 45 (can be 40~50) degree, the second acoustic conductance The pipe axis of pipe 442 is 90 (can be 85~95) degree with the angle of sensitive face.
Acoustic sensor 5 is microphone (or tuning fork, or poly meta fluoroethylene piezoelectric film), its output end and lock-in amplifier 6 input electrical connection.
The of the first passage 601 of lock-in amplifier 6, second channel 602 and the tapped off signal generator 1 of third channel 603 One signal output part 101, the signal output part 103 of secondary signal output end 102 and the 3rd, provide for receiving signal generator 1 Reference signal, with demodulate acoustic sensor 5 perception corresponding resonator in photoacoustic spectrum signals.
The tubulose acoustic resonant cavity of the shape of cylinder 7 is disposed thereon to be equipped with incidence window 421, exit window 422 and enters respectively In sample mouthful 411, outlet 412, and the photoacoustic cell 4 of preceding surge chamber 431, rear surge chamber 432.
When using, under test gas respectively enter tubulose acoustics via the injection port 411 and preceding surge chamber 431 on photoacoustic cell 4 First resonator 401 of resonator, the second resonator 402 and the 3rd resonator 403, and with approach its tubular cavity in through signal The first laser of first signal output part 101, secondary signal output end 102 and the modulation of the 3rd signal output part 103 of generator 1 After device light path 311, second laser light path 312 and the 3rd laser light path 313 interact, generate periodic pressure and become Change --- sound wave.The sound wave --- photoacoustic signal is conveyed by the first acoustic conducting pipe 441, the second acoustic conducting pipe 442 and the 3rd acoustic conducting pipe 443 On acoustic sensor 5 to its pipe port, thus photoacoustic signal is converted to and be sent to after electric signal lock and mutually put by acoustic sensor 5 The first passage 601 of device 6, second channel 602 and third channel 603, obtain as or are similar to the frequency characteristic in Fig. 4 greatly Three kinds of contents of component in shown under test gas.
Obviously, those skilled in the art can enter to triple channel acoustic resonant cavity optoacoustic spectroscopy sensing device of the invention The various changes of row and modification are without departing from the spirit and scope of the present invention.So, if to these modifications of the invention and modification Belong within the scope of the claims in the present invention and its equivalent technologies, then the present invention is also intended to exist comprising these changes and modification It is interior.

Claims (8)

1. a kind of triple channel acoustic resonant cavity optoacoustic spectroscopy sensing device, including the laser controller for being electrically connected with laser successively (2) and control signal source, and the tubulose acoustic resonant cavity that is communicated with acoustic conducting pipe coaxial with laser light path, it is placed in acoustic conducting pipe The lock-in amplifier (6) that the acoustic sensor (5) of port is electrically connected with acoustic sensor (5) output end, it is characterised in that:
The laser is first laser device (301), second laser (302) and the 3rd laser (303), its input tap First control output end (201) of laser controller (2), the second control output end (202) and the 3rd control output end (203);
The control signal source be signal generator (1), its first signal output part (101), secondary signal output end (102) and The respective input of the 3rd signal output part (103) tap laser controller (2);
The tubulose acoustic resonant cavity is by cylinder (7), its tubulose cavity axis with the first of cylinder (7) diameter parallel Resonator (401), the second resonator (402) and the 3rd resonator (403) composition, wherein, the first resonator (401) length L1, Relation between the second resonator (402) length L2 and the 3rd resonator (403) length L3 is L1<L3<L2, the first resonator (401), the radial direction angle between the 3rd resonator (403) and the second resonator (402) is 85~95 degree;
The acoustic conducting pipe is the first acoustic conducting pipe (441), the second acoustic conducting pipe (442) and the 3rd acoustic conducting pipe (443), first acoustic conductance The pipe port of pipe (441), the second acoustic conducting pipe (442) and the 3rd acoustic conducting pipe (443) is respectively positioned on the sensing of the acoustic sensor (5) On face, wherein, the first acoustic conducting pipe (441), the pipe axis of the 3rd acoustic conducting pipe (443) are 40~50 with the angle of the sensitive face Degree, pipe axis and the angle of the sensitive face of the second acoustic conducting pipe (442) are 85~95 degree;
The first passage (601) of the lock-in amplifier (6), second channel (602) and third channel (603) tap the signal First signal output part (101) of generator (1), secondary signal output end (102) and the 3rd signal output part (103), are used for The reference signal that signal generator (1) is provided is received, with the light acousto-optic in the corresponding resonator for demodulating acoustic sensor (5) perception Spectrum signal.
2. triple channel acoustic resonant cavity optoacoustic spectroscopy sensing device according to claim 1, it is characterized in that laser is half Conductor laser, or QCL, or optical parametric oscillation light source.
3. triple channel acoustic resonant cavity optoacoustic spectroscopy sensing device according to claim 1, it is characterized in that the first resonator (401) length L1 >=5cm, the second resonator (402) length L2≤35cm.
4. triple channel acoustic resonant cavity optoacoustic spectroscopy sensing device according to claim 1, it is characterized in that the first resonator (401), the tubular cavity diameter of the second resonator (402) and the 3rd resonator (403) is 1~15mm.
5. triple channel acoustic resonant cavity optoacoustic spectroscopy sensing device according to claim 1, it is characterized in that the first resonator (401), the center of the tubulose cavity axis of the second resonator (402) and the 3rd resonator (403) is on same circumference.
6. triple channel acoustic resonant cavity optoacoustic spectroscopy sensing device according to claim 1, it is characterized in that the first acoustic conducting pipe (441), the second acoustic conducting pipe (442) and the 3rd acoustic conducting pipe (443) respectively with the first resonator (401), the second resonator (402) and 3rd resonator (403) vertical connection, and its connectivity part is respectively positioned on the midpoint of corresponding resonator.
7. triple channel acoustic resonant cavity optoacoustic spectroscopy sensing device according to claim 1, it is characterized in that acoustic sensor (5) it is tuning fork, or microphone, or poly meta fluoroethylene piezoelectric film.
8. triple channel acoustic resonant cavity optoacoustic spectroscopy sensing device according to claim 1, it is characterized in that cylinder (7) shape Tubulose acoustic resonant cavity disposed thereon be equipped with incidence window (421), exit window (422) and injection port (411) respectively, go out sample In mouth (412), and the photoacoustic cell (4) of preceding surge chamber (431), rear surge chamber (432).
CN201510096806.XA 2015-03-04 2015-03-04 Triple channel acoustic resonant cavity optoacoustic spectroscopy sensing device Active CN104697933B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201510096806.XA CN104697933B (en) 2015-03-04 2015-03-04 Triple channel acoustic resonant cavity optoacoustic spectroscopy sensing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201510096806.XA CN104697933B (en) 2015-03-04 2015-03-04 Triple channel acoustic resonant cavity optoacoustic spectroscopy sensing device

Publications (2)

Publication Number Publication Date
CN104697933A CN104697933A (en) 2015-06-10
CN104697933B true CN104697933B (en) 2017-06-16

Family

ID=53345286

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201510096806.XA Active CN104697933B (en) 2015-03-04 2015-03-04 Triple channel acoustic resonant cavity optoacoustic spectroscopy sensing device

Country Status (1)

Country Link
CN (1) CN104697933B (en)

Families Citing this family (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN108593763B (en) * 2018-03-26 2021-03-30 山东大学 Real-time detection device for multi-component gas based on quartz tuning fork frequency division demodulation
CN111122445A (en) * 2018-11-01 2020-05-08 西安电子科技大学 Multiple resonance type T-shaped enhanced simultaneous detection method for multiple trace gases
CN111122444A (en) * 2018-11-01 2020-05-08 西安电子科技大学 Multiple resonant T-shaped enhanced multiple trace gas simultaneous detection device
CN113295628A (en) * 2020-02-23 2021-08-24 亘冠智能技术(杭州)有限公司 Device for simultaneously detecting black carbon, organic carbon and gas
CN112924388B (en) * 2021-01-22 2023-08-25 中国科学院合肥物质科学研究院 Orthogonal double-channel acoustic resonance device
CN112858184B (en) * 2021-01-29 2022-07-19 山西大学 Gas measuring device and method based on piezoelectric material
CN113109268B (en) * 2021-05-25 2022-07-01 武汉理工大学 Photoacoustic spectroscopy enhancement apparatus and method for gas detection using the same

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN200989883Y (en) * 2006-12-22 2007-12-12 中国科学院大连化学物理研究所 Optoacoustic Raman spectrum detector
CN102954948A (en) * 2011-08-26 2013-03-06 中国科学院安徽光学精密机械研究所 Gas sensor based on photoacoustic spectrometry
CN103760108A (en) * 2013-12-30 2014-04-30 浙江大学 Optoacoustic differential measurement method and device of humidity of wet steam
CN103837226A (en) * 2014-03-17 2014-06-04 山西大学 Double-resonant-cavity photoacoustic spectrophone and gas detection device using spectrophone

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7381954B2 (en) * 2005-09-29 2008-06-03 General Electric Company Apparatus and method for measuring steam quality
US8939006B2 (en) * 2011-05-04 2015-01-27 Honeywell International Inc. Photoacoustic detector with long term drift compensation

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN200989883Y (en) * 2006-12-22 2007-12-12 中国科学院大连化学物理研究所 Optoacoustic Raman spectrum detector
CN102954948A (en) * 2011-08-26 2013-03-06 中国科学院安徽光学精密机械研究所 Gas sensor based on photoacoustic spectrometry
CN103760108A (en) * 2013-12-30 2014-04-30 浙江大学 Optoacoustic differential measurement method and device of humidity of wet steam
CN103837226A (en) * 2014-03-17 2014-06-04 山西大学 Double-resonant-cavity photoacoustic spectrophone and gas detection device using spectrophone

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
基于光声光谱的变压器油中多组分气体检测方法;王新宽等;《山东电力技术》;20110315(第2期);第5-9页 *

Also Published As

Publication number Publication date
CN104697933A (en) 2015-06-10

Similar Documents

Publication Publication Date Title
CN104697933B (en) Triple channel acoustic resonant cavity optoacoustic spectroscopy sensing device
CN104237135B (en) CO gas detecting systems and method based on quartz tuning fork strengthened optoacoustic spectroscopy
CN102954948B (en) Gas sensor based on photoacoustic spectrometry
CN107064012B (en) Quartz enhanced photoacoustic spectroscopy gas-detecting device and method based on beat effect
CN105651374B (en) The coaxial optoacoustic spectroscopy acousimeter of single tube and the gas detection apparatus for using the acousimeter
CN107271368A (en) A kind of interior cavity-enhanced photo acoustic spectrum-type trace-gas sensors device
CN105259116A (en) Trace gas measurement device and method with adoption of photo-acoustic spectroscopy
CN103149156A (en) Double-channel light cavity ring-down atmospheric aerosol extinction instrument and extinction factor measuring method
CN103472002B (en) Photoacoustic spectroscopy gas detecting system in a kind of fiber laser cavity
CN105241814A (en) Apparatus and method for measurement of trace gas with photoacoustic spectroscopy technology
JPS595939A (en) Continuous measuring apparatus for particulate
CN203148832U (en) Double-channel cavity-ring-down atmospheric aerosol extinction instrument
CN104020114A (en) Method for analyzing trace concentration of ammonia gas
CN109269999A (en) A kind of infrared photoacoustic spectra detection system
US10876958B2 (en) Gas-detecting device with very high sensitivity based on a Helmholtz resonator
CN105466854A (en) Active air-chamber structure and photoacoustic spectrometry gas sensing system
CN107560730A (en) Bicavate photo-acoustic spectrometer
CN110927066B (en) Device and method for improving performance of photoacoustic spectrum sensor based on H-shaped resonance tube
CN108593763A (en) A kind of multicomponent gas real-time detection apparatus based on the demodulation of quartz tuning-fork frequency division
CN104880411A (en) Device with quartz tuning fork for detecting gas in resonant cavity
CN203534957U (en) Aerosol optical absorption coefficient detection device based on photoacoustic spectrum
CN113552212A (en) Radial cavity quartz enhanced photoacoustic spectrum sound detector and gas detection device thereof
CN103389270A (en) Apparatus for measuring concentration of trace gas, and method thereof
CN209495963U (en) A kind of infrared photoacoustic spectra detection system
CN103411904B (en) Based on the photoacoustic gas sensing device of poly meta fluoroethylene piezoelectric film

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant