1 00:00:00,008 --> 00:00:01,379 Analyticity. 2 00:00:01,379 --> 00:00:07,476 [MUSIC] 3 00:00:07,476 --> 00:00:10,536 Suppose f is a function and suppose that I 4 00:00:10,536 --> 00:00:14,046 can compute the derivative of f of 0 the second 5 00:00:14,046 --> 00:00:17,556 derivative of f of 0, the third derivative of 6 00:00:17,556 --> 00:00:21,280 f of 0, the fourth derivative of f of 0. 7 00:00:21,280 --> 00:00:21,931 And so on. 8 00:00:21,931 --> 00:00:24,895 Suppose that I can compute the nth derivative 9 00:00:24,895 --> 00:00:27,107 of f at 0 regardless of what n is. 10 00:00:27,107 --> 00:00:32,583 So in short, suppose that f is infinitely differentiable at 0, meaning that although 11 00:00:32,583 --> 00:00:35,321 might be really hard, atleast in principle 12 00:00:35,321 --> 00:00:38,448 I could compute the millionth derivative at 0. 13 00:00:38,448 --> 00:00:41,640 The billionth derivative at 0, I can compute any 14 00:00:41,640 --> 00:00:44,770 higher derivative that I want, at the point 0. 15 00:00:44,770 --> 00:00:49,440 Well then the power series for f around 0 is the sum n 16 00:00:49,440 --> 00:00:53,830 goes from 0 to infinity of the nth derivative of f at 0. 17 00:00:53,830 --> 00:00:57,570 This is a thing that makes sense, because f is infinitely differentiable. 18 00:00:57,570 --> 00:01:02,620 Divided by n factorial times x to the n. But what I don't know, is whether that 19 00:01:02,620 --> 00:01:08,560 power series converges to f, when x is near but not equal to zero. 20 00:01:08,560 --> 00:01:10,380 What I'm asking is whether this Taylor 21 00:01:10,380 --> 00:01:13,200 series is actually equal to the function, right? 22 00:01:13,200 --> 00:01:16,070 What's the relationship between this Taylor series 23 00:01:16,070 --> 00:01:18,550 and the original function that I'm studying? 24 00:01:18,550 --> 00:01:21,830 Sometimes it happens that the function is equal to its Taylor series. 25 00:01:21,830 --> 00:01:22,570 So let's give a name to 26 00:01:22,570 --> 00:01:26,070 that phenomenon. Here's how we're going to talk about this. 27 00:01:26,070 --> 00:01:27,830 The function f, which I'm assuming to 28 00:01:27,830 --> 00:01:30,680 be infinitely differentiable, is said to be real 29 00:01:30,680 --> 00:01:33,950 analytic at the point zero if there's some 30 00:01:33,950 --> 00:01:37,560 number big R positive, so that this happens. 31 00:01:37,560 --> 00:01:40,910 So that the function is equal to it's Taylor series. 32 00:01:40,910 --> 00:01:42,300 Maybe not everywhere. 33 00:01:42,300 --> 00:01:45,260 But at least when x is within big R of zero. 34 00:01:45,260 --> 00:01:47,800 I can make this a bit more general. 35 00:01:47,800 --> 00:01:49,580 Let's think for what this is really talking about, Right. 36 00:01:49,580 --> 00:01:52,250 What this definition is trying to get at is the idea 37 00:01:52,250 --> 00:01:55,690 that the function is equal to its tailor series around zero. 38 00:01:55,690 --> 00:01:57,550 That's what real analytic at zero means. 39 00:01:57,550 --> 00:02:01,380 It means the function has a power series representation around zero. 40 00:02:01,380 --> 00:02:05,900 When you generalize this and you talk about power series around other points. 41 00:02:05,900 --> 00:02:06,220 Alright. 42 00:02:06,220 --> 00:02:09,310 So, here's the definition of what it means for a function to 43 00:02:09,310 --> 00:02:13,170 be real analytic, not just at zero, but real analytic at some arbitrary 44 00:02:13,170 --> 00:02:14,400 point A. 45 00:02:14,400 --> 00:02:16,390 Well, it should still mean that there's some big R which will 46 00:02:16,390 --> 00:02:20,270 measure how for x is from a now, instead of from zero. 47 00:02:20,270 --> 00:02:22,630 And here I've written down the Taylor series around zero, 48 00:02:22,630 --> 00:02:25,240 but I should write down the Taylor series around a. 49 00:02:25,240 --> 00:02:30,180 So, instead of differentiating at zero, I'll differentiate f n times and 50 00:02:30,180 --> 00:02:34,360 evaluate at a, and then I'll multiply that not just by x. 51 00:02:34,360 --> 00:02:38,920 But by x minus a to the nth power. 52 00:02:38,920 --> 00:02:42,400 And then I don't want to say that x is close to zero. 53 00:02:42,400 --> 00:02:45,510 I want to say that x is within big R of a. 54 00:02:46,740 --> 00:02:52,260 So this is saying that at least near a, when you're within big R of a. 55 00:02:52,260 --> 00:02:54,640 F can be written as a power series. 56 00:02:54,640 --> 00:02:58,230 And that's what it means to say that f is real analytic at a point a. 57 00:02:58,230 --> 00:03:01,960 Let me draw a diagram to try to convey, you know, what is going on here. 58 00:03:01,960 --> 00:03:04,410 Let's suppose that this piece of paper represents 59 00:03:04,410 --> 00:03:07,680 all of the functions from the real numbers to the real numbers. 60 00:03:07,680 --> 00:03:10,180 And plenty of those functions are just miserable functions. 61 00:03:10,180 --> 00:03:11,650 Here's a graph of a terrible looking 62 00:03:11,650 --> 00:03:13,189 function, that's got a lot of discontinuities. 63 00:03:14,280 --> 00:03:16,620 Some of these functions though are continuous. 64 00:03:16,620 --> 00:03:20,320 So within the collection of all functions, I've got the continuous functions. 65 00:03:20,320 --> 00:03:22,730 Here's a graph of what looks like to be a continuous function. 66 00:03:22,730 --> 00:03:26,640 Still not great, because it's still got these spikes but at least it's continuous. 67 00:03:26,640 --> 00:03:30,050 Now some of these continuous functions are differentiable. 68 00:03:30,050 --> 00:03:33,330 A function as differentiable is necessarily continuous. 69 00:03:33,330 --> 00:03:36,294 So within the collection of all continuous functions, is a smaller 70 00:03:36,294 --> 00:03:38,374 collection just a differentiable functions, 71 00:03:38,374 --> 00:03:40,240 they don't have these terrible spikes. 72 00:03:41,330 --> 00:03:43,535 But just because you're differentiable, doesn't mean that 73 00:03:43,535 --> 00:03:46,840 you're say, twice differentiable or three times differentiable. 74 00:03:46,840 --> 00:03:49,300 So within the collection of all the differentiable functions, 75 00:03:49,300 --> 00:03:53,140 there's an even collection of functions which are infinitely differentiable. 76 00:03:53,140 --> 00:03:55,110 These are functions that I can differentiate once, 77 00:03:55,110 --> 00:03:56,040 twice, three times. 78 00:03:56,040 --> 00:03:59,320 These are functions I can differentiate as many times as I like. 79 00:03:59,320 --> 00:04:03,740 Sometimes people call these functions smooth functions or C infinity functions. 80 00:04:03,740 --> 00:04:06,610 This is a very restrictive class of functions. 81 00:04:06,610 --> 00:04:08,920 But there's an even more restrictive class of functions. 82 00:04:08,920 --> 00:04:12,270 Within the smooth functions, there's a smaller collection of functions. 83 00:04:12,270 --> 00:04:16,250 The real analytic functions. These functions aren't just smooth. 84 00:04:16,250 --> 00:04:16,440 Right? 85 00:04:16,440 --> 00:04:19,270 It's not just that I can differentiate these functions. 86 00:04:19,270 --> 00:04:20,400 These functions also 87 00:04:20,400 --> 00:04:23,620 have the property that if I write down their tailor series around 88 00:04:23,620 --> 00:04:29,130 some point, that tailor series converges near that point to the function. 89 00:04:29,130 --> 00:04:32,280 So these real analytic functions are really quite special. 90 00:04:32,280 --> 00:04:34,450 I mean, not every function is real analytic. 91 00:04:35,630 --> 00:04:39,199 And yet the surprise is that so many of the functions 92 00:04:39,199 --> 00:04:43,132 that we care the most about turn out to be real analytic. 93 00:04:43,132 --> 00:04:50,920 [NOISE] 94 00:04:50,920 --> 00:04:54,494 [SOUND]