1 00:00:00,090 --> 00:00:02,490 The following content is provided under a Creative 2 00:00:02,490 --> 00:00:04,059 Commons license. 3 00:00:04,059 --> 00:00:06,360 Your support will help MIT OpenCourseWare 4 00:00:06,360 --> 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 --> 00:00:17,290 from hundreds of MIT courses, visit MIT OpenCourseWare 7 00:00:17,290 --> 00:00:18,150 at ocw.mit.edu. 8 00:00:21,960 --> 00:00:24,540 PROFESSOR: The confocal resonator that we've looked at 9 00:00:24,540 --> 00:00:28,350 has many uses, and we'll illustrate one of them 10 00:00:28,350 --> 00:00:30,340 right now. 11 00:00:30,340 --> 00:00:37,350 So far, the laser frequency going into the cavity 12 00:00:37,350 --> 00:00:39,450 was only one frequency. 13 00:00:39,450 --> 00:00:41,640 We only had one frequency coming out the laser, 14 00:00:41,640 --> 00:00:44,820 because we selected it by means of the polarizer. 15 00:00:44,820 --> 00:00:49,050 Since the laser oscillates at several frequencies, at least 16 00:00:49,050 --> 00:00:52,170 two, at different polarization, then, again, 17 00:00:52,170 --> 00:00:58,620 by rotating the polarizer, I can select the other frequencies. 18 00:00:58,620 --> 00:01:03,990 So the cavity can be used as a spectrum analyzer. 19 00:01:03,990 --> 00:01:09,840 So if we look onto the scope, as I rotate the polarizer, 20 00:01:09,840 --> 00:01:12,660 you see that I can bring in other resonances. 21 00:01:12,660 --> 00:01:16,470 And these are not associated with transverse modes 22 00:01:16,470 --> 00:01:21,028 of the cavity, but they are associated with the frequencies 23 00:01:21,028 --> 00:01:21,570 of the laser. 24 00:01:21,570 --> 00:01:22,470 So here we are. 25 00:01:22,470 --> 00:01:26,610 Here is when the laser is operating single frequency 26 00:01:26,610 --> 00:01:28,260 going into the cavity. 27 00:01:28,260 --> 00:01:33,990 Now, I rotate the polarizer, and I admit the other frequencies 28 00:01:33,990 --> 00:01:37,110 from the laser, which are different polarizations. 29 00:01:37,110 --> 00:01:40,860 So in this way, the confocal resonator 30 00:01:40,860 --> 00:01:44,460 can be used as a spectrum analyzer. 31 00:01:44,460 --> 00:01:48,090 Now, in practice, you have to be careful in selecting 32 00:01:48,090 --> 00:01:51,600 the free spectral range of the resonator 33 00:01:51,600 --> 00:01:54,240 of the confocal cavity, so that there's 34 00:01:54,240 --> 00:01:59,150 no confusion about the separations in the frequencies 35 00:01:59,150 --> 00:02:02,200 of the light source. 36 00:02:02,200 --> 00:02:03,480 So here we are again. 37 00:02:03,480 --> 00:02:06,000 Here's when the laser single frequency 38 00:02:06,000 --> 00:02:09,419 going to the resonator. 39 00:02:09,419 --> 00:02:11,650 Here we have many frequencies. 40 00:02:11,650 --> 00:02:14,390 And if we had selected the free spectral range correctly, 41 00:02:14,390 --> 00:02:18,120 we would be able to measure exactly the spacing 42 00:02:18,120 --> 00:02:20,790 between the modes of the laser. 43 00:02:23,450 --> 00:02:30,740 So then, in conclusion, the set of demonstrations, 44 00:02:30,740 --> 00:02:34,160 we've looked at the plane parallel cavity, 45 00:02:34,160 --> 00:02:38,900 we've looked at the condition under which 46 00:02:38,900 --> 00:02:41,375 the modes superimpose. 47 00:02:41,375 --> 00:02:43,520 It was very touchy-- very touchy alignment 48 00:02:43,520 --> 00:02:45,170 with the plane parallel cavity. 49 00:02:45,170 --> 00:02:49,220 Then we looked at the cavity with curved mirrors. 50 00:02:49,220 --> 00:02:53,000 And we saw lots of transverse modes 51 00:02:53,000 --> 00:02:56,960 if we don't have the length of the resonator adjusted 52 00:02:56,960 --> 00:02:58,070 suitably. 53 00:02:58,070 --> 00:03:01,340 We also found that when the length of the resonator 54 00:03:01,340 --> 00:03:04,940 was equal to the radius of curvature of the mirrors 55 00:03:04,940 --> 00:03:07,220 in this case, the confocal condition, 56 00:03:07,220 --> 00:03:11,450 we found that the modes coalesced into two residences. 57 00:03:11,450 --> 00:03:17,120 And, finally, we showed how such a focal resonator 58 00:03:17,120 --> 00:03:22,280 can be used to analyze the spectrum of a light source 59 00:03:22,280 --> 00:03:24,670 like this laser.