Nanocar Race 2017: 3. The Tools – STM and AFM
This is a modal window.
The media could not be loaded, either because the server or network failed or because the format is not supported.
Formal Metadata
Title |
| |
Title of Series | ||
Part Number | 3 | |
Number of Parts | 163 | |
Author | ||
License | CC Attribution - NoDerivatives 4.0 International: You are free to use, copy, distribute and transmit the work or content in unchanged form for any legal purpose as long as the work is attributed to the author in the manner specified by the author or licensor. | |
Identifiers | 10.5446/50301 (DOI) | |
Publisher | 05jdrrw50 (ROR) | |
Release Date | ||
Language |
Content Metadata
Subject Area | ||
Genre | ||
Abstract |
| |
Keywords |
Beilstein TV8 / 163
16
20
31
43
44
47
51
57
67
78
102
105
112
131
135
138
139
140
144
145
146
149
150
151
154
157
159
160
161
162
163
00:00
Tidal raceMachinabilityComputer animationChemical experiment
00:15
Meeting/Interview
00:22
Chemical experiment
00:28
Meeting/Interview
00:35
Cell (biology)KnotChemical experiment
00:41
Sample (material)Chemical experiment
00:47
Surface scienceTiermodellChemical experiment
00:59
TiermodellChemical experiment
01:03
AageChemical experiment
01:22
Aage
01:28
Meeting/Interview
01:32
Atomic numberStuffingFermiumSample (material)Meeting/Interview
01:37
Surface scienceAtomic numberChemical experiment
01:45
Atomic numberChemical compound
01:49
AtomElectronic cigaretteSurface scienceChemical experimentMeeting/Interview
02:06
Sample (material)Chemical experiment
02:12
Sense DistrictMoleculeSample (material)Meeting/Interview
02:17
Sample (material)Chemical compoundChemical experiment
02:29
MoleculeComputer animation
02:33
Meeting/Interview
02:43
Spiro compoundComputer animation
02:46
ColourantZunderbeständigkeitThermoforming
03:01
VakuumverpackungSample (material)Ocean currentNahtoderfahrung
03:30
Sample (material)Electric currentGesundheitsstörungDiagram
03:45
Sample (material)Atomic numberSolutionElfMeeting/Interview
04:03
Sample (material)Computer animation
04:08
Sample (material)Atomic numberMeeting/Interview
04:19
AtomMoleculeTidal raceComputer animation
04:28
Tidal raceMeeting/Interview
Transcript: English(auto-generated)
00:02
We just talked about what a nanocar looks like. If you missed that video you will find it linked below. But how do you even know what such a small object looks like? Do you use a special machine for that or how does that work? Yeah, our nanocar is a size of only 1.5 nanometers. To see such a small object we need a very good microscope. I know microscopes from school,
00:23
we used those in biology class. Is it kind of like the same or what's the difference? It's not that kind of microscope. It's not a light microscope that you may have used in school classes. It's an STM that we use. So STM means scanning tunneling microscope and you can see it here. This is our STM. Okay, so you have to look in here, right? No, actually it does not work
00:43
like that. So you cannot look inside and see the image of the sample. What we do is we scan a tip over the surface and then we create an image of our nanocar. That's kind of hard to imagine. Yeah, maybe it's better if I explain it to you at the model. So let's go upstairs and
01:01
check how it works. Okay, let's go. So Nick, this is our STM model. Okay, I see. But it looks really old. It is old. So the STM was invented over 30 years ago, not far away from here in Switzerland at IBM. They also got the normal price for it and you can find the first
01:20
STM just next here. Okay, but it's already 30 years old and it's still in use. That must be a great technique. Yes, it is a great technique. It still gets really nice results. But how does it actually work? What you can see here is the tip and the sample. So all the ping pong bolts that you see are atoms. So the tip is constructed of four atoms and also the surface
01:48
has a lot of atoms. But that means that the tip of the tip is only made of one single atom. Exactly, and this is also a problem for the experiment. So we have to create a tip that has only one single atom at the apex. How do you do that? So we do that by crashing the tip into
02:05
the surface and then we pull the atoms out until one atom stays at the end. And then you move the tip across the sample, right? Exactly, and then we do a scanning with the tip over the sample and the tip follows the profile of the sample. And this profile of the sample is recorded by a
02:26
computer. You can see the line profile over there. But that's only one line, right? Because the molecule is three-dimensional and this is only one line. Yes, exactly. So we scan not only one line, we scan many lines, one after each other and out of that we get an image. And then
02:44
the image looks like that or what does it look like? No, actually the image looks different as you have seen downstairs in the lab. So we take the height information from these lines and then we put the color scale and with the colors you can see the height information. Okay, but how does the tip know when to move up and when to move down?
03:04
So for this we use the tunneling current between the tip and the sample. And the tunneling current is an effect of quantum mechanics. And it says that there is a small probability that an electron tunnels through a wall, which means from the sample to the tip. But the tip
03:23
never touches the sample, right? Exactly, this is because it's tunneling, so it tunnels through the wall without touching. And this effect is exponentially depending on the distance between tip and sample. And by this dependency we can control the distance and know if this tip has
03:43
to go up or to go down. But if we're talking about an electric current, that means that the sample you're trying to measure must be electrically conductive? Exactly, for STM this is a condition, so the sample has to be electrically conductive. And if it's not? If it's not, then we use a different
04:00
technique that is also very great, it's the AFM, atomic force microscope. And with this technique we don't use the tunneling current to control the tip sample distance, we use the forces between the atoms of the tip and the sample. Okay, are there any other benefits to the AFM? Yeah, of course the resolution is better, we can really see inside a molecule and resolve the
04:23
atomic structure of a molecule. So if the AFM has a higher resolution, why don't you just use that for the race as well? As you said, it's a race and we want to be fast, and by STM we can be much faster than by AFM. I see, so we just learned how we know where on the racetrack the nanocar actually is, but how do you control a nanocar? We'll learn about that in the next video, that
04:44
you will find, as always, linked below. I'll see you then, and have a good time. Bye-bye.