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  • So graphene is a kind of graphite? How, what's the... graphite, graphite looks like that

  • That's a big slab of graphite. I can by using the scotch tape method peel pieces off

  • The way I think of it

  • Is that a single atomic layer of graphite is graphene. I knocked it around a bit this be?

  • Single molar mono layer by layer graphene where you've got two layers held together by these Van der Waals forces

  • That's got slightly different electrical properties and then you've got tri layer and when you get up to 50 layers the graphene starts looking black

  • It's you seem to note that

  • one model layer of graphene over a wide part of the electromagnetic spectrum

  • Absorbs about 2% of the light intensity

  • incident on it

  • So it's very transparent and that makes it an interesting material as well because you got a transparent conductor

  • Amazingly the absorbance of graphene is given by the fine-structure constant

  • Times pi. Now, if any of you up to sixty symbols, you know, I'm fascinated with the fine-structure constant

  • You could see a sixty symbols video on that Andrei Guymon costume Novoselov isolated

  • graphene from a lump of graphite and

  • For some electrical contacts on and so that had some very interesting

  • Electrical properties they made a little transistor out of it

  • What we're waiting for now is to make lots of transistors

  • Out to reverse a much more difficult job that it's very difficult to switch off the channel

  • because of a bit of quantum mechanics that the

  • Electrons in graphene of this curious band structure graphene does not have a bandgap

  • like silicon or germanium or gallium

  • Arsenide a band gap is a gap in energy

  • If you want to get the electrons flowing, you've got to put the Fermi energy which tells you the energy of

  • the energy of the highest energy electron

  • you

  • Don't want that in in the middle of in the middle of the gap because then you don't get any free electrons or free holes

  • So you guys are gonna push the chemical potential down into the valence band or up into the conduction band

  • they stand bandgap is crucial for being able to turn off your silicon or gallium arsenide field effect transistor because in the

  • band gap between the conduction band and the valence band

  • Any electronic state so you could get in there and you can't put them in there by putting in some impurities. Those states are

  • Evanescent they decay very rapidly in space. So the electrons can't propagate through it when you're in the conduction band

  • About above the bandgap of the valence band below the bandgap the electrons or the missing electrons call the hole called the holes

  • Can move very very freely and had pretty good velocities, especially in something like indium phosphide or gallium arsenite that's faster than silicon

  • But silica has got this fantastic property

  • You can oxidize its surface and make silicon oxide now in addition to that, of course in the latest bunch of transits

  • He's not using silicon oxide

  • As the barrier you want a higher dielectric material

  • So you got like a hafnium salts and oxides that can that can push up that and you get more more electrons in your channel

  • For a given gate voltage. What's so exciting about graphene from my kind of looking forwards point of view. Well whereas silicon

  • or germanium

  • Or indium phosphide or gallium arsenide has a structure like this

  • It's a very rigid structure

  • Basically, the diamond structure for silicon silicon is just like diamond except the silica is replacing the carbon atoms. It's a very rigid structure

  • And the electrons can move freely in all three direct dimensions

  • The surface for MOSFETs the interface between the silicon and the oxide or the hafnium oxide

  • At that surface

  • you've got to be very careful because once you break these bonds and you're changing the chemistry at the atomic level and

  • You can have charge on those on those surface States that charge can be very adverse in principle. You can scatter electrons

  • scattering electrons randomize your momentum

  • so if you're trying to get them to move down a channel with a high current as quickly as possible to make if you wanna

  • switch a device class off if they zigzagging and knocking off impurities and so on till

  • They take longer to go down the device their mobility as it says is reduced

  • So you want it's nice to have a clean surface now the point about graphene. Is that graphene?

  • This is a lump of graphite

  • It looks very black. Of course

  • But you could take graphite and thin it down by exfoliation

  • Using the scotch tape method and I I just did exfoliate a little bit of graphene

  • Earlier this surface underneath the sellotape. It's not beginning to look a bit dirty. And those are layers of

  • Multi-layer graphite it's not necessarily single layer graphite. They may be five six ten 20 layers, but amongst all that

  • There will be a single model layer of

  • Graphene, so having it thin that's really important

  • Well having it thin is is interesting from a physical point of view because now we've got the electrons moving in

  • a single mono layer and they move

  • first of all at a very high speed

  • About five times faster than they would in gallium arsenide or indium

  • Phosphide three of three to five times faster anyway at a 10 to the 6 meters per second

  • Which is actually one 300 through the speed of light curiously enough, which is pretty fast. The problem is

  • That things like silicon germanium gallium arsenide and so on

  • These have a energy gap between the conduction band and the valence band

  • Any electron in that gap which are many because there not many states in the gap those electrons tell you get stuck now with graphene

  • There's no energy gap. It's a problem for switching off a transistor. You can't you can't switch it off with a conventional potential so

  • What the Manchester group decided to do?

  • They decided to go vertical so by combining what you need to do is two switches current off

  • so this you make a vertical tunnel transistor and a key element of the vertical tunnel transistor is

  • By getting a sister material to graphi and colleagues agonal boron nitride

  • It's got exactly the same crystal structure as graphene except that alternate atoms

  • if all of these are carbon atoms in Boran light or this one it would be

  • Boron, this will be nitrogen. This will be boron

  • this will be the nitrogen and so on going around here and that creates a very very strong barrier very effective and

  • powerful barrier a barrier in fact at six electoral votes

  • so six times the value of the electron gap in the energy gap in in gallium arsenide and so

  • in this device the

  • Graphene layer has put on top of it boron nitride and then on top of that we have another

  • graphene layer and we mount that on silicon silicon oxide and use the silicon as a gate electrode and you use that to

  • Control the tunnel current through the layer and using that device we were able to make a transistor in which you could switch off

  • So we were very excited about that

  • That work was published in in science and we were even more surprised and pleased that six weeks off

  • I think six weeks after our paper came out the Samsung group came up with a very similar concept

  • And they managed to put about a hundred of these transistors on a chip

  • so I think at that point everybody thought wow, these vertical devices are gonna take off but

  • Things do seem to have that doesn't seem to have happened. I think the technology is very

  • Difficult we to remember that it took

  • You know many beers decades for silicon to go from just an interesting lab based material

  • Into a field effect transistor and then into these incredible integrated circuits with all these transistors on a single chip

  • It takes a lot of time and it takes understanding the physics and understanding the material science

  • but in parallel with with all this work on graphene, I want to emphasize the graphene is one of a large family of

  • similar

  • two-dimensional materials in which you clinics which can be

  • Exfoliated and there are about I believe it around the thousand of these

  • Materials and one material that we are working on here in Nottingham and Manchester interesting as well is indium selenide

  • Molybdenum disulphide is none materials

  • Remember your Mali slip used to probably put on the gears of your bicycle on the gear wheels

  • That's a similar material because the molybdenum disulphide sheets can slide over each other with almost no friction

  • So this isn't that very hot material as well

  • Now those materials have got an energy gap and an energy gap that depends on

  • the number of atoms you make the crystal out of the great thing about

  • These layered compounds. Is that when you break them apart you

  • Break the band of ours bonds

  • these these bonds

  • don't get charged don't trap and don't become defects it looks as if

  • You know

  • the electron just doesn't get scattered off that so that's that's an interesting aspect of these devices that people are playing around with and

  • indium selenide

  • This is again a

  • Manchester knot in collaboration

  • we produced a feel effect transistor that has some really very good very very nice properties and that

  • Was published a few years ago and people that that indium selenide 'sister coppers are making quite a big impact at the moment

  • people are working away on it because it's like gap semiconductor and

  • you can combine it you can switch it off with using a field effect and you can also put make or a nitride barriers and

  • Not only that but then take one band of ours crystal

  • And then it take another exfoliation one on top of it and make a multiple sandwich structure with lots of layers and bread and butter

  • and so on and

  • They're all sleeping between properties that these materials could have good ab, so could be the EM facility, but not no no, no

  • No silicon has got years to go heist

  • I quite like when I my PhD I was spent ages trying to put good electrical contacts on silicon

  • And eventually the French colleague put very good contacts on and we were a very nice paper on the electronic properties in bulk silicon

  • But that's forgotten in the history of silicon, but back in

  • 1971-72

  • We looked at bonito photon resonance. Oh, I love silicon. I've got very got me interested in the field really and and curiously enough

  • I yes. I've almost forgotten this GC and Plessy were making very primitive

  • Feel effect transistors they were blimburn and reliable and we got our hands on some of these and we did some quite interesting

  • quantum experiments on the very first UK feel about transistors we couldn't get them from Germany or America, but

  • DC and Plessy were making material that materials. So no silicon is a great material. I'm not going to do it done

  • now I've got the token so I can lay the value in add the bay leaf emerged or into it and

  • Store it back and hand the target and now I've got the token again

  • I can load something into it into my register add something onto it back and pass the token on and I've got it

  • So I can load the value in add the value from a register story back

So graphene is a kind of graphite? How, what's the... graphite, graphite looks like that

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