Presentation on theme: "Coherent and Electro-Optics Research Group (CEORG)"— Presentation transcript:
1 Automated ADM with micrometer accuracy using the Michelson interferometer Coherent and Electro-Optics Research Group(CEORG)K Alzahrani, D Burton, M Lalor, F Lilley,F Bezombes, and M Gdeisat
2 Outlines Challenges Future work Conclusion Introduction Project objectiveBasic principlesMichelson interferometerADM using the Michelson interferometerChallengesFuture workConclusion
3 IntroductionConventional interferometry can only determine relative distance measurements – i.e. it can only determine how much further away one point is compared to another point, provided that both points are linked by a continuous path.Absolute distance interferometry (ADI)can measure the distance between any two arbitrary points.
4 Project objectiveBuilding a fully automated ADM system, with micrometer or better measurement accuracy, over comparatively large distances of up to 40 meters.
6 Interference Light consists of burst of sine waves. Two light waves derived from the same source and projected onto a point may interfere if interference conditions have been met.The interference could be constructive or destructive.
7 InterferenceSimilarly two light waves derived from the same source and projected onto a surface may also interfere to produce fringes if interference conditions have been met. As in Young’s double-slit experiment.
8 Coherence length Light source emits light as finite length trains. The phase of the sine wave changes randomly.The distance between two consecutive trains is called the coherence length.The longer the trains the more coherent the light source.40 m for the used laser.
9 Synthetic waveTwo light waves with different wavelengths, start with the same phase will become out of phase and then in phase regularly. We refer to the length over which this happens as synthetic wavelength s .s = (21/2-1 )
11 Michelson interferometer construction The Michelson interferometer produces interference fringes by splitting a beam of monochromatic light so that one beam strikes a fixed mirror and the other strikes a movable mirror.
12 Michelson interferometer Displacement measurement In a conventional displacement measurement, laser wavelength is held fixed and the interferometer system counts fringes as a reflector is displaced.
13 Michelson interferometer scenario.1 Laser operates at a fixed wavelength .Let l1=l2, grab 1st imagemove the adjustable mirrorto make l1≠l2,grab 2nd imageThere is a phase differencebetween both patterns .l =l1-l2l =0 then =0l = /4 then = πl = /2 then = 2π
14 Michelson interferometer scenario.2.a The arms of the interferometer is held fixed while the light wavelength is changed.Let l1=l2 , two fringe patterns are produces at 1 and 2. =0
15 Michelson interferometer scenario.2.b Let l1 ≠ l2, laser operates at 1 and 2Two fringe patterns are produced at 1 and 2.There is a phase shift between both fringe patterns.
16 The algorithmSuppose that we estimate lr and lm and we know l with precision of .Laser operates at 1,grab 1st imageLaser operates at 2,grab 2snd imagewe can determine l with accuracy of . Using the following equationl= N s + f s where f= /2πRepeating this routine several times with reduced we will determine l with increasing accuracy.
17 Example l ≃100mm,with =0.5mm. 1 =685nm grab the 1st image. 2 must satisfy the condition s = 2s = 1mm,δ =(1)/(s-1 )=0.47nm,2= nm grab 2nd imagemeasure =1.9 rads (0.3 s )ΔL must lie between 99.5mm and 100.5mm
18 N1=|l - /s | and N2=|l + /s | then N1=99 & N2=100. Combining these to and s, l 1 =99.3mm,l 2 =100.3mm.l 1 lies out of the tolerance range , therefore l =100.3mm2nd iteration /2=0.25mm,l lies between two values with 0.5mm difference. And according to N1 and N2 we choose one value that falls in the tolerance range and so on.Several iterations l can be determined with increasing accuracy.
22 System componentsA tunable laser with a tuning range of nm to 691 nm.The wavelength can be changed with an accuracy of 0.1 nm.A wavelength meter with an accuracy of nm.A monochrome camera with a resolution of 1024X1360 pixels.Michelson interferometer.
23 The absolute length measurement system The system is completely controllable from the computer. Using IDL software, we can set the tunable laser, read the wavelength and grab fringe patterns in less than one second. The tunable laser requires five seconds approximately to settle down.
24 AchievementsA significant amount of work has been put into building the system and calibrating it.An initial attempt was made to control the system using a semi-automated approach and it was partially successful.With the semi-automated system, setting the laser, reading the wavelength and grabbing an image takes at least 10 minutes for each iteration.The full iterative measurement process takes around two hours.
25 AchievementsVery recently, we managed to control the system completely from the IDL software.The system is now ready to use.With the IDL system, setting the laser, reading the wavelength and grabbing an image takes less than one second.The tunable laser requires five seconds approximately to settle down.The full iterative measurement process requires less than 30 seconds.
26 Future workThe use of multi-wavelengths instead of two wavelengths will be investigated.At the moment, we are able to measure the absolute distance for one point with m accuracy. This capability will be extended to measure the absolute distance for a surface.
27 ConclusionA new absolute length measurement system is proposed and a patent application is underway for this system.The hardware of the system has been built completely in GERI labs from scratch and is completely automated using IDL software.The operation principle has been verified mathematically and experimentally.The system offers 4 micrometers or better measurement accuracy over distances up to 40 meters.Future work will be carried out to improve the performance of this system and extend its capabilities.