In their study, Luican et al.4 find that, at small rotation angles, the local density of electronic states develops a dependence on position within the moirĂ©-pattern unit cell and no longer exhibits the Dirac-like, decoupled-layer, Landau-level pattern. Layer coupling becomes strong in this sense for rotation angles less than about 2°, corresponding to moirĂ©-pattern periods longer than about 10 nanometres. Here it is tempting to conjecture — from the spatial dependence of the density of electronic states — that bilayer wavefunctions have become localized, so that an STM measurement at one position reflects the stacking arrangement only at that position.
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The extraordinary sensitivity of the electronic properties of few-layer graphene systems to the relative orientations of their layers could prove useful in various applications, for example in ultra-sensitive strain gauges, pressure sensors or ultra-thin capacitors. Further progress requires an improved understanding of both large and small rotation-angle limits, and also improved experimental control of rotation angles.
The supreme task of the physicist is to arrive at those universal elementary laws from which the cosmos can be built up by pure deduction. There is no logical path to these laws; only intuition, resting on sympathetic understanding of experience, can reach them
Saturday, June 25, 2011
The mysterious Moire'- pattern-based electronic properties
Plenty of attention has been diverted to studying the bilayer graphene and hybrid structures consisting of patched mono-bi-layer graphene. A very fundamental problem in bi-layer graphene is how the electronic properties depend on the twisted angle. Theoretical study has been challenging. An interesting review in Nature on a recent PRL paper[http://www.nature.com/nature/journal/v474/n7352/full/474453a.html?WT.ec_id=NATURE-20110623#/references]:
labels:
domain textures,
electronics,
experiment,
graphene,
topological textures
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