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Stanford, IBM Team To Explore Spintronics
saxylife writes "NYTimes and various other media are carrying a story on the latest venture between IBM and Stanford," which will concentrate on spintronics, in other words, controlling "the magnetic orientation of atoms to store data.
It's supposed to ease the pressure of hitting the barrier of Moore's law."
Electrons can tunnel across a gate: can variables like spin do the same thing? If so, that's another barrier.
What this sounds like is a form of bubble memory, a "miracle" technology that was going to take over the world back in the day.
There were actully commercial parts made. But somebody killed it with their idea to have battery cmos ram. Then eeprom and flash memory came along.
They could actually make this work better with the refined manufacturing processes we have today. So I would not discount it out of hand.
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You're doing the same thing with 'traditional' electronics anyway. As things scale smaller and smaller, eventually the charge of a single electron will be the limiting factor within a bit, and even before that level is reached, fluctuations of several electrons could be large enough to cause things to "go awry" as you say.
The whole point of spintronics (or magnetoelectronics, it's less buzzword-trendy name) is to add an extra degree of freedom to electronics. Ie, instead of using components that switch on spin-independent electronic charge, one is now adding this extra component that can be switched/amplified/etc.
It's effectively opening up whole new doors, and spintronics represents the 2nd-rapidest movement of technology from lab to market (after the transistor, of course). The field is in its infancy right now, but has huge potential to revolutionize the types of electronic components that exist.
As you say, working on such nanoscale systems makes things really hard, and we're trying now to study and overcome these technical difficulties. But people are hopeful this will produce interesting devices, such as using the spin up/down eigenstates of the electron as the basis states for qubits in quantum computers, for example. Or many other quantum-dependent phenomena that are effectively averaged-out in standard electronics.
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