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LOS ANGELES — Give a graphene layer cake a twist and it superconducts — electrons flow freely through it without resistance. Made up of two layers of graphene, a form of carbon arranged in single-atom-thick sheets, the structure’s weird behavior suggests it may provide a fruitful playground for testing how certain unusual types of superconductors work, physicist Pablo Jarillo-Herrero of MIT reported March 7 at a meeting of the American Physical Society.
The discovery, also detailed in two papers published online in Nature on March 5, could aid the search for a superconductor that functions at room temperature, instead of the chilly conditions required by all known superconductors. If found, such a substance could replace standard conductors in various electronics, promising massive energy savings.
Layered graphene’s superconductivity occurs when the second layer of graphene is twisted relative to the first, at a “magic angle” of about 1.1 degrees, and when cooled below 1.7 kelvins (about –271° Celsius). Surprisingly, Jarillo-Herrero and colleagues report, the same material can also be nudged into becoming an insulator — in which electrons are stuck in place — by using an electric field to remove electrons from the material. That close relationship with an insulator is a characteristic shared by certain types of high-temperature superconductors, which function at significantly warmer temperatures than other superconductors, although they still require cooling.
Comprised of a lone hexagonal honeycomb lattice layer of tightly packed carbon atoms, graphene is one of the strongest, lightest, and most conductive compounds ever discovered. Bottom line, it’s an extraordinary composite.
However, a scientist from New York’s Clarkson University says he’s found a way to manufacture hemp waste into a material “better than graphene.” Moreover, the scientist — known to his peers as Dr. David Mitlin — says creating this graphene-like hemp material costs but a minuscule fraction of what it takes to produce graphene.
[...] By taking advantage of the complex multilayered structure of a hemp bast fiber precursor, such exquisite carbons were able to be achieved by simple hydrothermal carbonization combined with activation. This novel precursor-synthesis route presents a great potential for facile large-scale production of high-performance carbons for a variety of diverse applications including energy storage.
[...] Mitlin’s team built their supercapacitors using the hemp-derived carbons as electrodes and an ionic liquid as the electrolyte. Fully assembled, the devices performed far better than commercial supercapacitors in both energy density and the range of temperatures over which they can work. The hemp-based devices yielded energy densities as high as 12 Watt-hours per kilogram, two to three times higher than commercial counterparts. They also operate over an impressive temperature range, from freezing to more than 200 degrees Fahrenheit.
originally posted by: burgerbuddy
a reply to: Krakatoa
Room temp superconductor is awesome.
It will change everything.
originally posted by: Krakatoa
LOS ANGELES — Give a graphene layer cake a twist and it superconducts — electrons flow freely through it without resistance. Made up of two layers of graphene, a form of carbon arranged in single-atom-thick sheets, the structure’s weird behavior suggests it may provide a fruitful playground for testing how certain unusual types of superconductors work, physicist Pablo Jarillo-Herrero of MIT reported March 7 at a meeting of the American Physical Society.
The discovery, also detailed in two papers published online in Nature on March 5, could aid the search for a superconductor that functions at room temperature, instead of the chilly conditions required by all known superconductors. If found, such a substance could replace standard conductors in various electronics, promising massive energy savings.
Source: Give double-layer graphene a twist and it superconducts
Although this is an interesting finding, the next statement (in bold) seems a bit more relevant and exciting.
Layered graphene’s superconductivity occurs when the second layer of graphene is twisted relative to the first, at a “magic angle” of about 1.1 degrees, and when cooled below 1.7 kelvins (about –271° Celsius). Surprisingly, Jarillo-Herrero and colleagues report, the same material can also be nudged into becoming an insulator — in which electrons are stuck in place — by using an electric field to remove electrons from the material. That close relationship with an insulator is a characteristic shared by certain types of high-temperature superconductors, which function at significantly warmer temperatures than other superconductors, although they still require cooling.
Anyone else see the possibility for a relatively medium temperature superconducting transistor that has the ability to switch rapidly? If they can "productize" the twisting on a micro-scale, then it could lead to a superconducting integrated circuit design. And, i the research does find a way to increase the temps to standard room temperature, then the potential for a room temperature superconducting CPU & RAM memory would be theoretically possible.
Interesting research to follow for the next 5-10 years for sure.
What rule is that? I don't know of any rule against it, just that none have ever been observed, but if we keep experimenting with different materials, who knows what we might find?
originally posted by: badw0lf
I wish they'd stop making things and start making things.
but room temp superconductors breaks the old rule of them being unfeasable due to the super cooled environment in which they exhibit their super properties.
I don't know how you made the leap to relatively medium temperature on this graphene topic, because as far as I know the temperature for this effect is very low.
originally posted by: Krakatoa
Anyone else see the possibility for a relatively medium temperature superconducting transistor that has the ability to switch rapidly?
If Eremets and colleagues are right, then other hydrogen compounds may be good candidates for high-temperature superconductivity too. For instance, other researchers have published theory papers on arXiv suggesting compounds that pair hydrogen with platinum, potassium, selenium or tellurium, instead of sulfur.
Taking a slightly different tack, Zhang in Dallas and Yugui Yao of the Beijing Institute of Technology in China predict that substituting 7.5% of the sulfur atoms in hydrogen sulfide with phosphorus and upping the pressure to 2.5 million atmospheres (250 GPa) could raise the superconducting transition temperature all the way to 280 K6, which is above water's freezing point.
originally posted by: Arbitrageur
What rule is that? I don't know of any rule against it, just that none have ever been observed, but if we keep experimenting with different materials, who knows what we might find?
originally posted by: badw0lf
I wish they'd stop making things and start making things.
but room temp superconductors breaks the old rule of them being unfeasable due to the super cooled environment in which they exhibit their super properties.
I don't know how you made the leap to relatively medium temperature on this graphene topic, because as far as I know the temperature for this effect is very low.
originally posted by: Krakatoa
Anyone else see the possibility for a relatively medium temperature superconducting transistor that has the ability to switch rapidly?
There are other more promising materials for "relatively medium temperature" superconductors as you put it, as described in this article:
Superconductivity record sparks wave of follow-up physics
If Eremets and colleagues are right, then other hydrogen compounds may be good candidates for high-temperature superconductivity too. For instance, other researchers have published theory papers on arXiv suggesting compounds that pair hydrogen with platinum, potassium, selenium or tellurium, instead of sulfur.
Taking a slightly different tack, Zhang in Dallas and Yugui Yao of the Beijing Institute of Technology in China predict that substituting 7.5% of the sulfur atoms in hydrogen sulfide with phosphorus and upping the pressure to 2.5 million atmospheres (250 GPa) could raise the superconducting transition temperature all the way to 280 K6, which is above water's freezing point.
I'm not holding my breath for room temperature graphene superconductors since there seem to be more promising alternative materials for that, but it's still some interesting research at very low temperatures.
In April 2018, a group at MIT in the U.S. showed that it is possible to generate a form of superconductivity in a system of two layers of graphene under very specific conditions. To do this, the two hexagonal nets must be twisted against each other at a 1.1 degree angle. Under this condition, a flat band forms in the electronic structure. The preparation of samples from two layers of graphene with such an exactly adjusted twist is complex, and not suitable for mass production. Nevertheless, the study has attracted a lot of attention among experts.
At BESSY II, the physicists are able to scan the so-called band structure of the sample. This band structure provides information on how the charge carriers are distributed among the quantum-mechanically permitted states and which charge carriers are available for transport at all. The angle-resolved photoemission spectroscopy (ARPES) at BESSY II enables such measurements with extremely high resolution.
Via an exact analysis of the band structure, they identified an area that had previously been overlooked. "The double layer of graphene has been studied before because it is a semiconductor with a band gap," explains Varykhalov. "But on the ARPES instrument at BESSY II, the resolution is high enough to recognize the flat area next to this band gap."
"It is an overseen property of a well-studied system," says first author Dr. Dmitry Marchenko. "It was previously unknown that there is a flat area in the band structure in such a simple well-known system."
This flat area is a prerequisite for superconductivity, but only if it is situated exactly at the so-called Fermi energy. In the case of the two-layer graphene, its energy level is only 200 milli-electron volts below the Fermi energy, but it is possible to raise the energy level of the flat area to the Fermi energy either by doping with foreign atoms or by applying an external voltage, the so-called gate voltage.
The physicists have found that the interactions between the two graphene layers and between graphene and the silicon carbide lattice are jointly responsible for the formation of the flat band area. "We can predict this behavior with very few parameters and could use this mechanism to control the band structure," adds Oliver Rader.
A silicon carbide crystal is heated until silicon atoms evaporate from the surface, leaving first a single-layer of graphene on the surface, and then a second layer of graphene. The two graphene layers are not twisted against each other, but lie exactly on top of each other.
Our high-resolution ARPES study of BLG on 6H-SiC shows that the band structure around the Embedded Image point has neither the predicted parabolic nor the Mexican hat shape but stays in an intermediate stage causing flat band dispersion. The band has a number of unusual properties such as very high photoemission intensity, very high DOS without detectable dispersion and narrow width, contribution of only one graphene sublattice, and the absence of photoemission interference effects. We explain the mechanism of the flat band appearance and show that, by influencing sublattice and interlayer asymmetries, one can radically control the band shape and its properties. Indications of enhanced electron-phonon coupling, together with the discussed possibility of creating and controlling the flat band, are related to the question of high-temperature superconductivity in graphene- and graphite-based systems, while, on the other hand, the mechanism of the flattening of the dispersion is more universal and could be used in transport applications beyond BLG.
Over the past years, theory has consistently predicted flat band superconductivity accessible by doping or gating and with enhanced critical temperature.