1 00:00:00,120 --> 00:00:02,490 MAN: The following content is provided under a Creative 2 00:00:02,490 --> 00:00:04,059 Commons license. 3 00:00:04,059 --> 00:00:06,350 Your support will help MIT OpenCourseWare 4 00:00:06,350 --> 00:00:10,720 continue to offer high quality educational resources for free. 5 00:00:10,720 --> 00:00:13,350 To make a donation or view additional materials 6 00:00:13,350 --> 00:00:17,300 from hundreds of MIT courses, visit MIT OpenCourseWare 7 00:00:17,300 --> 00:00:18,480 at OCW.mit.edu. 8 00:00:20,792 --> 00:00:22,500 SHAOUL EZEKIEL: This demonstration, we're 9 00:00:22,500 --> 00:00:27,570 going to show the influence of an optical fiber 10 00:00:27,570 --> 00:00:31,616 on the polarization properties of light. 11 00:00:31,616 --> 00:00:37,080 In this case, we're going to use a normal single mode fiber. 12 00:00:37,080 --> 00:00:40,540 The setup is as shown here. 13 00:00:40,540 --> 00:00:42,090 We have a helium neon laser. 14 00:00:42,090 --> 00:00:45,090 Here's the beam from the laser reflected by this mirror 15 00:00:45,090 --> 00:00:48,960 here, then by another mirror here, 16 00:00:48,960 --> 00:00:53,690 into a quarter-wave plate and a polarizer. 17 00:00:53,690 --> 00:00:58,380 And, in this way, by rotating the polarizer here, 18 00:00:58,380 --> 00:01:01,110 I can select any linear polarization 19 00:01:01,110 --> 00:01:03,780 I want in this region. 20 00:01:03,780 --> 00:01:07,795 Then what we do is we take the light from here, 21 00:01:07,795 --> 00:01:09,990 we pass it through a short focal length lens, 22 00:01:09,990 --> 00:01:14,250 focus it into the fiber to the single mode fiber over here, 23 00:01:14,250 --> 00:01:17,070 and then the output of the fiber is, again, 24 00:01:17,070 --> 00:01:20,310 [INAUDIBLE] by another short focal length lens, 25 00:01:20,310 --> 00:01:22,830 and then the output of this lens, 26 00:01:22,830 --> 00:01:27,490 and we let go onto the screen. 27 00:01:27,490 --> 00:01:29,640 So this is the basic setup, now we're 28 00:01:29,640 --> 00:01:34,170 ready to look at polarization effects in fibers. 29 00:01:34,170 --> 00:01:39,840 Now, first, we have to establish the state of polarization 30 00:01:39,840 --> 00:01:42,360 of the light going into the fiber. 31 00:01:42,360 --> 00:01:44,880 What I'm going to do, take this polarizer 32 00:01:44,880 --> 00:01:47,630 and place it over here. 33 00:01:47,630 --> 00:01:53,100 And then I'll take a card, place it here. 34 00:01:53,100 --> 00:01:58,990 And now I want to rotate the polarizer and the axis. 35 00:01:58,990 --> 00:02:01,682 The little white arrow here indicates the transmission axis 36 00:02:01,682 --> 00:02:02,390 of the polarizer. 37 00:02:02,390 --> 00:02:07,980 So I can rotate polarizer now, and then 38 00:02:07,980 --> 00:02:13,390 in this region over here I have now, 39 00:02:13,390 --> 00:02:17,100 which means that the state of polarization of light 40 00:02:17,100 --> 00:02:21,180 is orthogonal to the direction of this arrow. 41 00:02:21,180 --> 00:02:24,420 So indeed we have plane-polarized light as 42 00:02:24,420 --> 00:02:27,750 indicated by the arrow over here, which 43 00:02:27,750 --> 00:02:30,170 is orthogonal to the one here. 44 00:02:30,170 --> 00:02:32,276 All right, so now we've established the-- 45 00:02:32,276 --> 00:02:38,470 that the state of polarization is linear going into the fiber. 46 00:02:38,470 --> 00:02:40,500 Now, let's look at the polarization of the light 47 00:02:40,500 --> 00:02:42,200 coming out of the fiber. 48 00:02:42,200 --> 00:02:45,690 Again, I'm going to take the polarizer 49 00:02:45,690 --> 00:02:48,930 and place it over here, the output. 50 00:02:52,460 --> 00:02:57,110 And now let's look at the spot in the inset. 51 00:02:57,110 --> 00:02:58,730 Here we have the spot in the inset. 52 00:02:58,730 --> 00:03:01,580 Now, I'm going to rotate the transmission 53 00:03:01,580 --> 00:03:05,852 axis of the polarizer to see what we have. 54 00:03:05,852 --> 00:03:09,042 Gee, we have indeed plane-polarized light 55 00:03:09,042 --> 00:03:10,250 also coming out of the fiber. 56 00:03:10,250 --> 00:03:12,470 So we have plane-polarized light going in 57 00:03:12,470 --> 00:03:17,350 and plane-polarized light coming out. 58 00:03:17,350 --> 00:03:22,310 Now, to demonstrate what the fiber does 59 00:03:22,310 --> 00:03:27,290 to the polarization in a very dramatic way, all I have to do 60 00:03:27,290 --> 00:03:35,150 is twist the fiber by just pushing on it. 61 00:03:35,150 --> 00:03:39,830 And you can see that now, just by applying a little stress 62 00:03:39,830 --> 00:03:40,950 to the fiber-- 63 00:03:40,950 --> 00:03:43,070 now I have changed the polarization 64 00:03:43,070 --> 00:03:47,960 because now I have light coming out of the polarizer 65 00:03:47,960 --> 00:03:52,120 while before it was not. 66 00:03:52,120 --> 00:03:55,650 Now, again, I can push the fiber around some more. 67 00:03:55,650 --> 00:03:58,787 As you can see, I can change the amount 68 00:03:58,787 --> 00:04:00,620 of light coming through the polarizer, which 69 00:04:00,620 --> 00:04:02,690 means that this state of polarization 70 00:04:02,690 --> 00:04:07,610 is changing just by simply applying simple stress. 71 00:04:07,610 --> 00:04:11,120 I can apply mechanical stress like I'm doing now. 72 00:04:11,120 --> 00:04:20,029 I can get the similar effect by heating the fiber and so on 73 00:04:20,029 --> 00:04:25,130 so that the state of polarization 74 00:04:25,130 --> 00:04:32,810 then can be influenced quite a bit by the environment-- 75 00:04:32,810 --> 00:04:35,180 the effect of the environment on the fiber. 76 00:04:35,180 --> 00:04:38,660 You can see here I can make it come out 77 00:04:38,660 --> 00:04:41,340 very bright through the polarizer when originally it 78 00:04:41,340 --> 00:04:41,840 was not. 79 00:04:41,840 --> 00:04:45,140 Here we are [INAUDIBLE] now zero, 80 00:04:45,140 --> 00:04:46,970 which it means plane polarized. 81 00:04:46,970 --> 00:04:50,150 Now, it's some state of polarization. 82 00:04:50,150 --> 00:04:51,680 In fact, I'm going to hold it-- 83 00:04:51,680 --> 00:04:54,620 hold the fiber in this position, and then now I'm going to go 84 00:04:54,620 --> 00:04:57,200 and I'm going to turn the polarizer to see indeed 85 00:04:57,200 --> 00:05:00,950 do I have plane-polarized light or elliptically 86 00:05:00,950 --> 00:05:01,760 polarized light. 87 00:05:04,900 --> 00:05:07,000 Well, it's elliptically polarized light 88 00:05:07,000 --> 00:05:09,870 because I can't [INAUDIBLE]. 89 00:05:09,870 --> 00:05:12,170 So now I have changed this state of polarization 90 00:05:12,170 --> 00:05:16,570 then from linear to elliptical. 91 00:05:16,570 --> 00:05:23,680 And, again, if I put more stress on the fiber, 92 00:05:23,680 --> 00:05:26,350 let's see now what state polarization I get now? 93 00:05:26,350 --> 00:05:28,300 Again, you can see it is elliptical because I 94 00:05:28,300 --> 00:05:32,620 can't [INAUDIBLE]. 95 00:05:32,620 --> 00:05:37,300 So in conclusion then, the-- a single mode-- 96 00:05:37,300 --> 00:05:41,290 irregular single mode fiber can change the state 97 00:05:41,290 --> 00:05:45,690 the polarization of light going into it into almost anything, 98 00:05:45,690 --> 00:05:47,550 to plane polarized, circular polarized, 99 00:05:47,550 --> 00:05:48,880 elliptically polarized. 100 00:05:48,880 --> 00:05:54,370 And this is influenced greatly by the environment 101 00:05:54,370 --> 00:05:56,950 that the fiber is in. 102 00:05:56,950 --> 00:06:00,130 So it's very difficult to maintain then 103 00:06:00,130 --> 00:06:05,050 a good state of polarization or a known state of polarization 104 00:06:05,050 --> 00:06:08,260 in a single mode fiber because of these environmental 105 00:06:08,260 --> 00:06:10,520 disturbances. 106 00:06:10,520 --> 00:06:14,800 If one wants to maintain, let's say, linear polarization, 107 00:06:14,800 --> 00:06:18,960 one would have to use a polarization maintaining fiber.