[0:00] This video is sponsored by Incogn. I [0:02] made this rubber band that changes color [0:04] when you stretch it. It's cool, isn't [0:05] it? It starts off blue, then goes green, [0:08] and then red, and then when I let go, it [0:11] returns back to blue. And it's the same [0:13] mechanism that's used in this [0:15] 135year-old photography technique that's [0:18] halfway between a hologram and a [0:20] photograph. It's the same chemistry as [0:23] black and white photography. But look, [0:25] when I change the viewing angle, it [0:27] bursts into color. And this isn't just [0:29] any color image. It's arguably the [0:32] truest color image you'll ever see. And [0:34] that's because standard color [0:36] photography is a lie. That's a bit [0:38] inflammatory, isn't it? Helps with the [0:40] views. All right. Here's why standard [0:43] color photography is a scam. So, when [0:45] you take a picture of something yellow, [0:47] let's say, then you've got yellow light [0:50] hitting the sensor of the camera. And [0:53] that light has a wavelength of about 580 [0:56] nanome. But when you look at the [0:58] resulting image, you're not getting that [1:01] wavelength coming from the image. [1:04] Instead, you're getting some red [1:05] wavelengths and some green wavelengths [1:08] that your brain interprets as yellow. [1:11] And that's because we don't have [1:12] dedicated cone cells in our eyes for [1:16] yellow wavelengths of light. Whereas, [1:18] when I look at this image, all the [1:20] wavelengths of light that were hitting [1:22] the plate when the picture was taken are [1:24] now hitting my eyes as I look at it. And [1:27] that's because it's basically a hologram [1:29] except it's encoding color information [1:32] instead of depth information. For the [1:34] vast majority of people, you'd never be [1:35] able to tell, but we can use this [1:37] spectrum analyzer to see it. So look, [1:40] this is my phone screen through a [1:41] spectrum analyzer. And as I move around [1:44] the image, what you're seeing is just [1:46] three peaks changing in height. That's [1:49] red, green, and blue. And they match up [1:51] with the three types of cones in our [1:53] eyes. But when I point it at the Litman [1:55] plate, you can see this complex [1:57] distribution of wavelengths. And because [1:59] there are flowers in this image, we're [2:01] even getting a bit of ultraviolet there [2:03] as well. Actually, that's a good point. [2:05] Standard photography doesn't work for [2:06] other animals, like bees, for example, [2:09] because they have a different [2:11] distribution of cones in their eyes. And [2:14] actually, even for a tiny minority of [2:16] humans that have four different cone [2:18] cells and the neurological machinery to [2:21] use the extra one, the yellow in this [2:23] Litman plate will look like the yellow [2:25] they see in real life, whereas yellow in [2:27] standard photographs would look wrong. [2:29] So, how is it that this black and white [2:31] film can reproduce the full spectrum of [2:34] colors from the real world? Well, [2:36] they're called Litman plates, and they [2:38] were made for me by an amazing [2:39] photographer called John Hilty. I really [2:42] hope you'll check out his stuff. I'll [2:44] leave a link to it in the description. [2:46] And once I had them in my hands, I just [2:48] thought, well, I have to show this to [2:49] the world. So, here we are. We're going [2:51] to figure out together why color seems [2:54] to magically emerge from this plate. [2:57] Here's a clue to start with. Watch what [2:59] happens when I breathe on this plate. [3:02] See how the whole rainbow seems to shift [3:05] to the left? Why the heck does it do [3:07] that? Well, surprisingly enough, it's [3:09] for the same reason that chameleons [3:11] change color. Watch this. [3:16] Yeah, that didn't work. I don't know why [3:18] I thought that would work. Anyway, we'll [3:20] get back to chameleons later, I promise. [3:22] But let's use this rubber band of mine [3:25] first. We'll call it synthetic chameleon [3:27] skin because it too changes color for [3:30] the same reason that a Lipman plate [3:32] changes color when it's breathed on. So, [3:34] the way I made this rubber band is I [3:36] pulled the DVD apart and poured some [3:39] silicon on this exposed surface inside. [3:42] In other words, I used that surface as a [3:44] mold. The surface looks really flat, but [3:47] it's actually covered in tightly packed [3:48] grooves. So, now my rubber band also has [3:51] these tiny grooves in it. And it's these [3:54] tiny grooves that bring the colors out. [3:57] So, again, it's not color pigment like [4:00] the silicon doesn't have any color of [4:02] its own. It's transparent. Instead, the [4:04] color comes from the structure of the [4:06] surface. That's why it's called [4:08] structural color. And that means if you [4:10] can change the structure by stretching [4:13] it, for example, then you can change the [4:15] color. How cool is that? How a Lithuan [4:18] play ends up with structural color is [4:20] amazing. But first, what is structural [4:22] color? Well, my favorite example is [4:25] bubbles. Why do you get rainbows in [4:27] bubbles? Well, let's zoom right in on [4:30] the bubble film and see what happens [4:31] when light shines on it. Some light gets [4:34] reflected and some light gets [4:35] transmitted from that top surface. Then [4:38] some gets reflected and some gets [4:39] transmitted from that bottom surface. [4:42] And then some gets reflected and some [4:44] gets transmitted from the top surface. [4:46] Again, suppose this is red laser light [4:48] we're shining here. And this is the [4:50] wavelength. Now, it just so happens that [4:52] this distance here is exactly one full [4:55] wavelength of the red light. So you can [4:58] see that the peaks and the troughs line [5:00] up perfectly. So when you add them [5:02] together, you get an even bigger wave. [5:04] That's called constructive interference. [5:06] But what if we switch to a blue laser? [5:08] Well, now this distance is one full [5:11] wavelength and a half. So now the peaks [5:14] of this wave line up with the troughs of [5:17] this wave and vice versa. So when you [5:19] add them together, they exactly cancel [5:21] out and you get no light coming out. [5:24] That's called destructive interference. [5:26] Now, for in between wavelengths, you [5:29] wouldn't get perfectly constructive [5:31] interference or perfectly destructive [5:33] interference. So, you'd get a brightness [5:35] in between for intermediate wavelengths. [5:39] Except what's actually happening here is [5:41] the light is bouncing up and down inside [5:44] this soap film multiple times. What does [5:48] that mean for those in between [5:49] wavelengths? Well, when you add up loads [5:52] of offset waves like this, it ends up [5:55] looking like complete destructive [5:57] interference anyway. In other words, [5:59] when you have lots of reflections, the [6:01] interference becomes really selective [6:03] and it gets tighter the more reflections [6:06] there are. So, you end up seeing only [6:08] that one perfect wavelength of red light [6:11] that exactly matches and a little bit [6:13] either side. And the reason you see [6:15] rainbows is because the angle that the [6:19] light enters the film at changes this [6:22] length. So here red light is reflected [6:25] and here blue light is reflected and you [6:28] get the full spectrum between these two [6:30] points. So that also explains why DVDs [6:33] have rainbows in them except that [6:35] instead of the light bouncing up and [6:37] down inside a thin film of soapy water, [6:40] you've got light that's reflecting off [6:41] closely packed ridges. So actually the [6:44] same thing is true for my rubber band. [6:45] You see different colors at different [6:47] angles. The difference is that I can [6:49] shift the rainbow by stretching it. And [6:51] that makes sense because when it's [6:53] stretched those ridges become more [6:55] spread out and so the wavelengths that [6:57] constructively interfere become longer. [7:00] And the same thing happens when a [7:02] chameleon changes color. So a chameleon [7:04] has these special cells called [7:05] iridaphors that are packed full of these [7:09] tiny regularly spaced crystals of [7:12] guanine. When the crystals are tightly [7:14] packed, they cause constructive [7:15] interference for blue light and [7:17] destructive interference for all the [7:20] other wavelengths. But a chameleon is [7:21] able to engorg these cells by changing [7:24] the osmotic pressure. When the cells [7:26] expand, the crystals move further apart [7:30] from each other. This causes the [7:32] crystals of guanine to spread out so [7:34] that they constructively interfere [7:37] longer wavelengths of light. That's not [7:40] the whole story though. Like chameleons [7:42] also have a pigment layer. So the final [7:44] color that you see is a mixture of [7:47] structural color that the chameleon can [7:49] tune and this pigment color. Real [7:52] chameleon skin differs from my synthetic [7:54] chameleon skin in a couple of ways. The [7:56] first is that with my synthetic [7:58] chameleon skin, the interference is [7:59] happening because of surface ridges. [8:01] Whereas with real chameleon skin, the [8:03] diffraction is happening through deeper [8:05] and deeper layers into the skin. The [8:07] other difference is that real chameleon [8:09] skin isn't iridescent, which is actually [8:11] really impressive. Like, if there's [8:12] diffraction going on, why don't I see [8:14] the color change when the viewing angle [8:17] changes like it does with this mother of [8:20] pearl or this peacock feather? It's [8:23] actually a bit easier to see how moro [8:25] butterflies do it. That incredible blue [8:28] is also structural color. And just like [8:31] the chameleon, it looks blue from all [8:33] angles. To see why, you have to look [8:36] under an electron microscope. This is a [8:38] cutaway through the wing. Here's a [8:40] diagram of it for simplicity. So, the [8:43] interference comes from these ridges [8:45] here. So, if light comes directly down, [8:48] it interferes with this stack of [8:50] branches, and they're spaced for blue [8:53] light. Now, if all the branches from the [8:55] neighboring trees lined up like this, [8:58] we'd get iridescent. Because look, when [9:01] light comes in at an angle, it can [9:03] bounce off this top branch, then the [9:06] second from top branch on this [9:08] neighboring tree and so on. And each gap [9:10] is the same distance. So you've got [9:13] constructive interference for say red [9:16] when viewed at this angle. But cleverly, [9:18] the moro butterfly has all these trees [9:21] offset randomly at different heights [9:23] from each other. So when light comes in [9:25] at an angle, it doesn't see regularly [9:28] spaced reflectors. it sees a random [9:30] mess, so constructive interference is [9:33] impossible. So, you only get reflected [9:35] light when it's coming straight down, [9:36] and that's always blue. Chameleons do a [9:39] similar thing with those guanine [9:41] crystals, but it's not as easy to [9:43] visualize. But anyway, we finally come [9:45] full circle back to the Litman plate. [9:48] So, when I breathed on the back of this [9:49] Lipman plate, the gel on the back [9:51] absorbed some of the moisture from my [9:53] breath and expanded. And so just like [9:55] the crystals inside the chameleon skin, [9:58] the structures inside this plate [10:00] expanded and separated when engorged [10:03] with water. And that separation causes [10:06] the color to shift. But what are these [10:08] structures inside the Litman plates? And [10:10] how did they get there? To figure it [10:12] out, let's look at how one of these [10:14] pictures is taken. First, take a sheet [10:16] of glass and coat it in a photographic [10:19] emulsion. This emulsion is made of [10:21] gelatin with lots of teeny tiny crystals [10:24] embedded in it. These are tiny grains of [10:27] silver haloid, meaning a latis of silver [10:30] and something like broomemide. You then [10:32] put the plate face down in a bath of [10:35] mercury. I don't have any mercury, so [10:37] you'll have to use your imagination. [10:38] Now, let's see what happens when the [10:39] plate is put in a camera and exposed to [10:42] light. In particular, we'll zoom right [10:44] in and see what happens when yellow [10:46] light hits this little section of the [10:49] plate. First, it passes through the [10:51] emulsion from the front and then it gets [10:53] reflected off the mercury bath and then [10:56] it passes back through the emulsion from [10:59] the back. And crucially, the reflected [11:01] light interferes with the incoming light [11:04] and that creates a standing wave. You [11:06] know, standing waves, right? The [11:08] important thing is you've got light [11:09] energy here at the antinodeses and no [11:12] light energy here at the nodes. And so [11:15] these crystals here at the antinodeses [11:18] start to absorb photons. And eventually [11:21] as a result, some of the atoms in those [11:23] crystals break away from the halite [11:25] atoms and form metallic silver flakes. [11:28] Just over here, the plate is maybe being [11:31] exposed to blue light instead. Blue [11:33] light has a shorter wavelength. So these [11:35] bands of exposed crystals are closer [11:38] together. In other words, the color of [11:40] the light is encoded into the spacing [11:42] between these bands. After the image is [11:44] exposed, the plate is developed. And [11:46] this bit is really clever. So you've got [11:48] this emulsion with silver haly crystals [11:51] in it. And some of these crystals have [11:53] little silver flakes in them from the [11:55] exposure. And these silver flakes act [11:58] like a catalyst during development. so [12:01] that any crystal that contains even a [12:03] tiny amount of metallic silver becomes [12:06] entirely metallic silver by the end. [12:09] There's a final step that flushes away [12:11] all the silver haly that didn't get [12:14] converted into metallic silver and what [12:17] you're left with is lots of tiny silver [12:20] mirrors embedded in gelatin. Then to [12:23] view the plate, you just shine white [12:25] light onto it. And every time the light [12:27] hits one of the mirrors, some gets [12:29] reflected and some gets transmitted down [12:32] to the next mirror and so on. And just [12:34] like with the soap bubble and the [12:37] chameleon and the butterfly, the [12:39] resulting interference produces a [12:41] specific color that depends on the [12:43] spacing of the mirrors. In other words, [12:45] the Litman plate contains a defraction [12:48] grating that encodes all of the spectral [12:52] information from the original scene. So [12:54] why does it only work when it's [12:56] illuminated from certain angles? Well, [12:59] with normal pigments, you have light [13:02] scattering. So white light can hit the [13:04] pigment from any direction. Some of it [13:07] gets absorbed, some of it gets [13:08] scattered, and some of that scattered [13:10] light reaches your eyes. But when light [13:13] scatters off a Litman plate, you don't [13:15] get interference. So you see it as black [13:17] and white. It's only when the light [13:19] reflects off the surface that you see [13:22] the color. Which is why when I shift the [13:24] focus of my camera lens here, you can [13:26] see that the light source is reflected [13:29] there in the plate. You know, Litman [13:31] plates have their drawbacks. Reprints [13:34] are basically impossible. Exposure times [13:38] run to minutes. the restricted viewing [13:41] angle is less than ideal and they can [13:45] get a bit washed out if you don't get [13:47] the process exactly right which is [13:50] probably why pigment-based RGB [13:53] photography eventually came to dominate. [13:56] So, Lipman plates might feel like a [13:58] historical culde-sac, but it turns out [14:01] that holograms like this one that can be [14:04] viewed with reflected white light are a [14:07] direct descendant of Litman plates. So, [14:11] you know, thank you, Gabriel Litman. You [14:14] deserved that Nobel Prize. Right, [14:16] massive tangent. I love scams. What I [14:19] mean is, well, I'm interested in [14:21] everything, including scams. So, when I [14:24] get a scam phone call, I try and keep [14:26] them on the phone as long as possible [14:27] because I'm interested to know like what [14:29] are their tactics and stuff like that. I [14:30] don't particularly recommend it cuz you [14:32] could end up giving away something [14:34] unintentionally. But let's have a look [14:36] at an example. This is a phone call from [14:38] my bank. So, you're [14:42] >> Yes, you [14:46] wigs. I thought you'd know my address. [14:48] >> No, I can send you over a text message [14:50] now. [14:52] Yeah. Okay. It's interesting to see how [14:54] they socially engineer their way around [14:57] various safety features built into the [14:59] banking app. For example, there's a big [15:00] banner in the app that basically says [15:03] we're not calling you. So like if the [15:05] bank isn't calling me, who the hell are [15:07] you? [15:07] >> Yeah, it's just Okay, I'm just telling [15:09] you now. It says here, you've never [15:11] spoke we've never spoken to you on the [15:12] phone. [15:13] >> Yeah, that's correct, sir. That's what [15:14] we've got added onto your account cuz if [15:16] somebody else has logged in, they can [15:18] see when's the last time you've been on [15:19] the call with us here, sir. Maybe you're [15:21] seeing some red flags here. But the [15:23] thing that gave it away perhaps more [15:24] than anything was just how frustrated he [15:27] was getting with me. Anyway, carry on. [15:28] So, what what what do you need me to do? [15:31] >> Are you recording the call, you [15:34] >> I'm not recording it. Are you genuinely [15:38] >> Are you sure you're not recording? [15:41] >> This guy that wasn't very convincing. I [15:43] just don't think my bank would speak to [15:45] me like that. It became clear from the [15:47] call that they had my bank details, [15:49] which was worrying. And I actually [15:51] figured out how they must have got it [15:52] because while he was trying to persuade [15:54] me of his legitimacy, he read out my [15:56] email address, but the email address was [15:58] wrong. It's not the one from the [16:00] account. It's a random one that I hardly [16:01] ever use. But I remember I did use it [16:04] recently for a specific transaction on a [16:07] camping website. So my guess is that the [16:09] caller must have used something like SQL [16:11] injection on that camping website to get [16:13] my car details. But anyway, every time [16:15] you put your details into an online [16:17] form, you're hoping that the company [16:18] behind it has good security. Obviously, [16:22] that's not always the case. So, it's a [16:24] good idea in general to try and minimize [16:28] how many companies have our data. The [16:30] good news is that our data has been [16:32] consolidated to a large extent by these [16:34] middleman companies. So, if you can get [16:36] your data off their databases, it can't [16:38] trickle down to all the others. Not only [16:40] would you be less vulnerable to data [16:42] breaches, you'd also get fewer spam [16:44] calls. The bad news is there are [16:47] hundreds of these middleman companies [16:49] called data brokers. And they all have [16:51] different procedures for requesting data [16:53] removal. Honestly, if one person could [16:55] just sit down and do all the hard work [16:58] of figuring out how to interact with all [17:01] of these different companies to remove [17:02] their data, well, I'd happily pay them a [17:05] little bit of money to do the same thing [17:06] for my data since they've already done [17:09] all the research. And of course, that's [17:11] exactly what I've done. I'm talking [17:13] about Incogn, the sponsor of this video. [17:16] It's super easy. You give them your [17:18] details, you give them permission to act [17:19] on your behalf, and then they just go [17:21] away and do it. They also do people [17:23] search sites, which is reassuring. And [17:25] on the unlimited plan, you can do custom [17:27] removal requests if you find your data [17:30] anywhere out there in the wild. I did it [17:33] because it turns out that past Steve was [17:35] doxing future Steve. So, while you might [17:37] not be able to protect yourself from [17:39] every camping website that hasn't [17:41] sanitized its inputs, you can protect [17:43] yourself from data brokers and people [17:45] search. If you're interested, the offer [17:47] on this one is really good. Go to [17:48] incognite.com/science [17:50] and use code science at checkout to get [17:53] 60% off an annual membership. The link [17:56] is also in the description, so check out [17:58] Incogn today. I hope you enjoyed this [18:00] video. If you did, don't forget to hit [18:01] subscribe and the algorithm thinks [18:03] you'll enjoy this video next. [18:07] What's that?