CN2927040Y - Interference measuring device of solid laser medium heat distortion - Google Patents

Interference measuring device of solid laser medium heat distortion Download PDF

Info

Publication number
CN2927040Y
CN2927040Y CN 200620044116 CN200620044116U CN2927040Y CN 2927040 Y CN2927040 Y CN 2927040Y CN 200620044116 CN200620044116 CN 200620044116 CN 200620044116 U CN200620044116 U CN 200620044116U CN 2927040 Y CN2927040 Y CN 2927040Y
Authority
CN
China
Prior art keywords
laser
laser medium
spectroscope
spectroscopy
light
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
CN 200620044116
Other languages
Chinese (zh)
Inventor
刘佳
付文强
胡企铨
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.)
Shanghai Institute of Optics and Fine Mechanics of CAS
Original Assignee
Shanghai Institute of Optics and Fine Mechanics 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 Shanghai Institute of Optics and Fine Mechanics of CAS filed Critical Shanghai Institute of Optics and Fine Mechanics of CAS
Priority to CN 200620044116 priority Critical patent/CN2927040Y/en
Application granted granted Critical
Publication of CN2927040Y publication Critical patent/CN2927040Y/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Images

Landscapes

  • Investigating Or Analysing Materials By Optical Means (AREA)

Abstract

The utility model discloses an interference measuring device for dynamic thermal distortion of solid-state laser medium, which comprises a He-Ne laser, a beam expander telescope, a first spectroscopy, a second spectroscopy, a first totally reflecting mirror, a second totally reflecting mirror, an observation screen, a CCD detector, and a computer; wherein, the He-Ne light produced by the He-Ne laser is divided into two beams by the first spectroscopy after passing through the beam expander telescope, a beam of the reflected light is reflected by the first totally reflecting mirror, then by the second spectroscopy after passing through the solid-state laser medium, the other reflected light passes through the second spectroscopy after being reflected by the second totally reflecting mirror, the two beams of light are interfered on the semi reflecting surface of the second spectroscopy, the interference pattern is imaged on the observation screen and are collected and then sent into the computer by the CCD detector to process data. The utility model is has the advantages of simple structure, easy manufacture, low cost and dynamic measurement of the temperature distribution of the slab laser medium without contact.

Description

The interferometric measuring means of solid laser medium dynamic heat distortion
Technical field
The utility model relates to laser medium, particularly a kind of interferometric measuring means of solid laser medium dynamic heat distortion.
Background technology
The distortion of working-laser material heat is to hinder the key factor that laser power further improves and obtain high light beam quality.Therefore effectively in real time the dynamic heat distortion of detection laser medium fully, is in depth understood the Temperature Distribution of working-laser material, and it is effectively compensated, to guarantee great-power solid laser continuously, efficient operation is very important.
In the heat distortion research of solid state laser, great majority all are Temperature Distribution, the thermal stress that the mode of employing numerical simulation is analyzed laser medium, [the thermal effect research of LD profile pump Nd:YAG laser instruments such as Zhang Ling such as thermal focal, laser and infrared, 2003, Vol.33, No.1], but can not obtain the Temperature Distribution of laser medium really and accurately.The heat distortion that utilizes interference technique exploring laser light medium that the also has [interference testing of YAG laser bar optical pumping dynamic thermal effect such as Luo Bikai, Chinese laser, 1993, Vol.A20, No.3], but only be used under the situation of monopulse pumping, and what obtain is three-dimensional skiodrome, does not obtain temperature profile.Also utilize in the pumping process, reference light is in the other end incident of laser crystal pumping, after the reflection of front/rear end, interfere mutually, [interferometric method such as Yang Yongming is measured LD end pumping Nd:YAG crystal thermal focal length to the thermal focal length of measuring crystal according to moving of taking place of the interference fringe that produces, the photon journal, in February, 2005, Vol.34, No.2], but adopt the degree of accuracy of this method not high.In a word, the Temperature Distribution of all failing in experiment, dynamically to measure laser medium of prior art, and do not have real-time, and handle more satisfactoryization, precision is not high.
Summary of the invention
The purpose of this utility model is to provide a kind of interferometric measuring means of solid laser medium dynamic heat distortion, and claimed structure is simple, debugs easily, can obtain the dynamic heat distortion of laser medium.
Technical solution of the present utility model:
A kind of interferometric measuring means of solid laser medium dynamic heat distortion, it is characterized in that laser instrument by He-Ne, beam expanding telescope, first spectroscope, second spectroscope, first total reflective mirror, second total reflective mirror, film viewing screen, ccd detector and computing machine are formed, the position relation of said modules is as follows: the He-Ne light that the He-Ne laser instrument sends is divided into two bundles through behind the beam expanding telescope by first spectroscope, a branch of transmitted light is reflected by first total reflective mirror through the laser medium of solid state laser, reflect through second spectroscope again, another folded light beam is through the second total reflective mirror reflecting ﹠ transmitting, second spectroscope, this two-beam interferes on second spectroscopical semi-reflective surface, interference pattern is imaged on the film viewing screen, and the interference fringe pattern is sent into computing machine by the ccd detector collection and carried out data processing.
Because the thermal effect that the measured laser medium produces during by pumping can change the refractive index of laser medium, and change of refractive will make the optical path difference by laser medium change, the interference fringe generation deformation that causes producing is with mobile, utilize ccd detector to take the interference fringe dynamic changing process continuously, obtain a series of interference fringe images according to time sequence.By analyzing these interference fringe pictures, calculate the change of refractive situation according to every bit on these bar graphs at the corresponding constantly progression that moves of difference, and calculate the heat distortion situation of laser medium according to change of refractive.For the more accurate fringe order that moves that obtains every bit correspondence on the striped, thereby adopted the way of Flame Image Process, through some steps such as image pre-service, adopt thinning algorithm to extract the skeleton that extracts striped at last, this brings great convenience for follow-up data processing.
Be example with side pump slab laser below, concrete computation process is as follows: set up the coordinate system (see figure 2), the length of establishing the slab laser medium is L, and the wavelength of surveying light (He-Ne light) is λ, and the refractive index of half bar medium of pumping is not n 0, axial (z axle) refractive index gradient is zero after the pumping, cross section (x-y plane) gone up index distribution and is:
n=n(x,y) (1)
Corresponding point (x, the variable quantity of optical path difference y) be Δ l (x, y), the striped number that moves past be Δ m (x, y), the change of refractive amount be Δ n (x y), has so:
Δl(x,y)=Δm(x,y)·λ (2)
And have:
Δl(x,y)=[n(x,y)-n 0]·L=Δn(x,y)·L (3)
Contrast (2) (3) two formulas have so:
Δn ( x , y ) = Δm ( x , y ) · λ L - - - ( 4 )
The change of refractive amount that just can calculate according to the striped amount of movement like this.The temperature variation that temperature refraction rate coefficient dn/dt causes be the thermic refractive index change delta n (x, main cause y) are therefore approximately thought:
Δn ( x , y ) = Δn ( x , y ) T = ΔT ( x , y ) · ( dn dt ) - - - ( 5 )
Comprehensive above-mentioned two formulas (4), (5) then have:
ΔT ( x , y ) = Δn ( x , y ) / ( dn dt ) - - - ( 6 )
So just can obtain the slab laser medium by the Temperature Distribution in the pumping process, and also can directly obtain three-dimensional skiodrome from interference fringe.
Advantage of the present utility model or technological achievement are:
1, in the utility model, owing to adopt the method for interference fringe, the computer image processing technology of maturation is applied to handle striped, can access higher precision.
2, in the utility model,, can not influence the operate as normal of laser instrument because employing is the metering system of noncontact.
3, in the utility model,, can calculate the heat distortion situation etc. that change of refractive obtains laser medium because the interference fringe of ccd detector collection can import and handle in the computing machine and calculate.
4, in the utility model, because used device architecture is simple, whole device is stable to be used, and is convenient to processing and manufacturing.
Description of drawings
Fig. 1 is the structured flowchart of the interferometric measuring means of the utility model solid laser medium dynamic heat distortion.
Fig. 2 is the slab laser medium synoptic diagram of profile pump.
Concrete embodiment
Consult Fig. 1, Fig. 1 is the structured flowchart of the interferometric measuring means of the utility model Laser Measurement medium dynamic heat distortion.The interferometric measuring means of the utility model solid laser medium dynamic heat distortion as seen from the figure, by He-Ne laser instrument 1, beam expanding telescope 2, first spectroscope 3, second spectroscope 7, first total reflective mirror 6, second total reflective mirror 8, film viewing screen 11, ccd detector 10 and computing machine 12 are formed, the position relation of said modules is as follows: the He-Ne light that He-Ne laser instrument 1 sends is divided into two bundles through beam expanding telescope 2 backs by first spectroscope 3, a branch of transmitted light is reflected by first total reflective mirror 6 through the laser medium 5 of solid state laser, again through 7 reflections of second spectroscope, another folded light beam is through second total reflective mirror, 8 reflecting ﹠ transmittings, second spectroscope 7, this two-beam interferes on the semi-reflective surface of second spectroscope 7, and interference pattern is imaged on the film viewing screen 11, and the interference fringe pattern is gathered and sent into computing machine 12 and carry out data processing by ccd detector 10.
The laser that sends from He-Ne laser instrument 1 enters interferometer light path through beam expanding telescope 2, and the laser medium 5 in the light path collects the width of cloth interference fringe picture of this moment not by pumping by ccd detector 10 at this moment, preserves bar graph as a setting.
When pumping source 4 and 9 pairs of laser medium 5 beginning pumpings, gather storage by the interference fringe on the film viewing screen 11 of ccd detector 10 real-time continuous and send into computing machine 12, till pumping finishes.
Number for convenience of moving interference fringes on the accurate Calculation cross section, fringe center is handled and extracted to all interference fringes that collect, the a series of interference fringes and the background striped that collect during then with pumping compare, and analysis meter is calculated three-dimensional wave face, Temperature Distribution, equivalent thermal focal etc.
Having adopted a block size among embodiment of the utility model is the process of tabular laser glass simulated laser diode (LD) the pumping laser slab of 2cm*3cm*1cm, change two LD laser instruments 4,9 into two sides that two refrigerating sheets stick on laser glass, the experimental situation temperature is 20 ℃.Adopt the temperature of two refrigerating sheets of temperature control circuit control, its temperature difference is remained on about 60 ℃, the heat transfer process when simulating lath by pumping.
Put up light path earlier, clap a width of cloth background bar graph.Then laser glass is put into light path, ccd detector 10 was gathered 12 seconds altogether with the process of the moving interference fringes on the speed continuous acquisition film viewing screen 11 of per second 25 frames when refrigerating sheet is started working, and at this moment heat transfer process is basicly stable.
For the progression that more accurate calculating striped moves, must extract the center of striped earlier, according to the Theoretical Calculation of front, can obtain the dynamic heat distortion situation of this laser glass in heat transfer process.Show from experimental result: the result conforms to Theoretical Calculation, the utlity model has simple in structure, be easy to make, with low cost, can under non-contacting condition, the Temperature Distribution to the slab laser medium carry out kinetic measurement, and in pumping continuously, monopulse pumping or repetition pulse pumping, can both measure, be widely used.

Claims (1)

1, a kind of interferometric measuring means of solid laser medium dynamic heat distortion, it is characterized in that by He-Ne laser instrument (1), beam expanding telescope (2), first spectroscope (3), second spectroscope (7), first total reflective mirror (6), second total reflective mirror (8), film viewing screen (11), ccd detector (10) and computing machine (12) are formed, the position relation of said modules is as follows: the He-Ne light that He-Ne laser instrument (1) sends is divided into two bundles through beam expanding telescope (2) back by first spectroscope (3), a branch of transmitted light is reflected by first total reflective mirror (6) through the laser medium (5) of solid state laser, reflect through second spectroscope (7) again, another folded light beam is through second total reflective mirror (8) reflecting ﹠ transmitting second spectroscope (7), this two-beam interferes on the semi-reflective surface of second spectroscope (7), interference pattern is imaged on the film viewing screen (11), and the interference fringe pattern is sent into computing machine (12) by ccd detector (10) collection and carried out data processing.
CN 200620044116 2006-07-21 2006-07-21 Interference measuring device of solid laser medium heat distortion Expired - Fee Related CN2927040Y (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN 200620044116 CN2927040Y (en) 2006-07-21 2006-07-21 Interference measuring device of solid laser medium heat distortion

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN 200620044116 CN2927040Y (en) 2006-07-21 2006-07-21 Interference measuring device of solid laser medium heat distortion

Publications (1)

Publication Number Publication Date
CN2927040Y true CN2927040Y (en) 2007-07-25

Family

ID=38281293

Family Applications (1)

Application Number Title Priority Date Filing Date
CN 200620044116 Expired - Fee Related CN2927040Y (en) 2006-07-21 2006-07-21 Interference measuring device of solid laser medium heat distortion

Country Status (1)

Country Link
CN (1) CN2927040Y (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102003936A (en) * 2010-09-14 2011-04-06 浙江大学 Method and device for simultaneously measuring droplet position, particle sizes and complex refractive index
CN103901624A (en) * 2012-12-25 2014-07-02 鸿富锦精密工业(深圳)有限公司 Laser projection apparatus
CN104502068A (en) * 2014-12-30 2015-04-08 工业和信息化部电子第五研究所 Device and method for detecting weak absorption of optical element
CN113401860A (en) * 2021-05-25 2021-09-17 杭州电子科技大学 Self-radiating chip and temperature measuring device and method thereof

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102003936A (en) * 2010-09-14 2011-04-06 浙江大学 Method and device for simultaneously measuring droplet position, particle sizes and complex refractive index
CN102003936B (en) * 2010-09-14 2012-01-04 浙江大学 Method and device for simultaneously measuring droplet position, particle sizes and complex refractive index
CN103901624A (en) * 2012-12-25 2014-07-02 鸿富锦精密工业(深圳)有限公司 Laser projection apparatus
CN104502068A (en) * 2014-12-30 2015-04-08 工业和信息化部电子第五研究所 Device and method for detecting weak absorption of optical element
CN113401860A (en) * 2021-05-25 2021-09-17 杭州电子科技大学 Self-radiating chip and temperature measuring device and method thereof

Similar Documents

Publication Publication Date Title
CN1888839A (en) Solid laser dynamic heat distortion interference measuring device
CN102788558B (en) Three-dimensional deformation measuring system and three-dimensional deformation measuring method combining speckle correlation and speckle interference
CN103528524B (en) The method of acoplanarity displacement field distribution inside perspective measurement polymer matrix composites
CN102252823B (en) Dual-wavelength phase-shift interference-based method for measuring optical heterogeneity
CN102332956B (en) Dispersion compensation method for broadband light source
CN101806723B (en) Double-beam multi-functional z scanning optical non-linear measuring device and method
CN101308091B (en) Method for measuring optical non-linear 4f phase coherent imaging
CN102679950B (en) Distance measuring device and method based on three-wavelength femtosecond laser
CN1357100A (en) Laser-ultrasonic measurement of wall thickness
CN105891434A (en) Seawater salinity online detection method and device
CN104296678B (en) Heterodyne interferometer based on phase shift of low-frequency-difference acousto-optic frequency shifter
CN104596989A (en) Method for measuring refractive index distribution of transparent medium on basis of interference fringe image processing
CN103412299A (en) Femtosecond laser absolute distance measuring device and method based on non-linear optical sampling
CN105044035B (en) Refractive index and thickness method for synchronously measuring and system based on spectral domain interferometer
CN2927040Y (en) Interference measuring device of solid laser medium heat distortion
CN110057543B (en) Wave surface measuring device based on coaxial interference
CN202748011U (en) Three-dimensional deformation measurement system with speckle correlation and speckle interference combined
CN105571517A (en) Modified coherence peak demodulation method for fiber end face detection
CN107064067A (en) The measuring system and method for a kind of air refraction profile of dual interferometer
CN102865810B (en) Orthogonal double-grating based detecting device for synchronous phase shift common-light path interference and detecting method therefor
CN205003080U (en) Refracting index and thickness synchronous measurement system based on spectral domain interferometer
CN104792269B (en) A kind of calculation method of the fiber end face height value insensitive to linear phase-shift error
CN101493311A (en) Idle running error automatic compensation apparatus for laser heterodyne interferometer
CN102221535B (en) Three-vacuum-tube-based gas refraction index measurer
CN102840823B (en) Common-path interference detecting device based on beam-split synchronism phase shifting and detecting method

Legal Events

Date Code Title Description
C14 Grant of patent or utility model
GR01 Patent grant
C17 Cessation of patent right
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20070725