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Automated ADM with micrometer accuracy using the Michelson interferometer 1 Coherent and Electro-Optics Research Group (CEORG) K Alzahrani, D Burton, M.

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Presentation on theme: "Automated ADM with micrometer accuracy using the Michelson interferometer 1 Coherent and Electro-Optics Research Group (CEORG) K Alzahrani, D Burton, M."— Presentation transcript:

1 Automated ADM with micrometer accuracy using the Michelson interferometer 1 Coherent and Electro-Optics Research Group (CEORG) K Alzahrani, D Burton, M Lalor, F Lilley, F Bezombes, and M Gdeisat

2 Outlines 2 Introduction Project objective Basic principles Michelson interferometer ADM using the Michelson interferometer Challenges Future work Conclusion

3 Introduction 3 Conventional 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 4 Project objective Building a fully automated ADM system, with micrometer or better measurement accuracy, over comparatively large distances of up to 40 meters.

5 Basic principles 5 Interference Coherence length Synthetic wavelength

6 Interference 6 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 Interference 7 Similarly 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 Youngs double-slit experiment.

8 Coherence length 8 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 wave 9 Two 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 = ( 2 1 / )

10 Synthetic wave formation 10 1 = 100nm, 2 =120nm s =600nm

11 Michelson interferometer construction 11 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 12 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 13 Laser operates at a fixed wavelength. Let l 1 =l 2, grab 1 st image move the adjustable mirror to make l 1 l 2,grab 2 nd image There is a phase difference between both patterns. l =l 1 -l 2 l =0 then =0 l = / 4 then = π l = / 2 then = 2 π

14 Michelson interferometer scenario.2.a 14 The arms of the interferometer is held fixed while the light wavelength is changed. Let l 1 =l 2, two fringe patterns are produces at 1 and 2. =0

15 Michelson interferometer scenario.2.b 15 Let l 1 l 2, laser operates at 1 and 2 Two fringe patterns are produced at 1 and 2. There is a phase shift between both fringe patterns.

16 The algorithm 16 Suppose that we estimate l r and l m and we know l with precision of. Laser operates at 1,grab 1 st image Laser operates at 2,grab 2 snd image we can determine l with accuracy of. Using the following equation l= N s + f s where f= /2 π Repeating this routine several times with reduced we will determine l with increasing accuracy.

17 Example 17 l 100mm,with =0.5mm. 1 =685nm grab the 1 st image. 2 must satisfy the condition s = 2 s = 1mm, δ =( 1 )/( s - 1 )=0.47nm, 2 = nm grab 2 nd image measure =1.9 rads (0.3 s ) Δ L must lie between 99.5mm and 100.5mm

18 N1=| l - / s | and N2=| l + / s | then N 1 =99 & N 2 =100. Combining these to and s, l 1 =99.3mm, l 2 =100.3mm. l 1 lies out of the tolerance range, therefore l =100.3mm 2 nd 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. 18

19 Algorithm flowchart 19

20 20

21 Results 21

22 22 A 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. System components

23 23 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. The absolute length measurement system

24 24 A 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. Achievements

25 25 Very 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. Achievements

26 26 The 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. Future work

27 27 A 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. Conclusion

28 Thank you Any Questions 28


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