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·îÉϼ¸Æª2012 science ÉÏÓйØgrapheneµÄÎÄÏ×£¬Çë´ó¼ÒÅõ³¡£¡·ÅÐÄÏÂÔØ£¬²»Ðè½ð±Ò¹þ£¡ ÏÂÔØÁË£¬¶¥Ò»ÏÂok£¡ 1¡¢Electromechanical Properties of Graphene Drumheads £»Science 336, 1557 (2012); We determined the electromechanical properties of a suspended graphene layer by scanning tunneling microscopy (STM) and scanning tunneling spectroscopy (STS) measurements, as well as computational simulations of the graphene-membrane mechanics and morphology. A graphene membrane was continuously deformed by controlling the competing interactions with a STM probe tip and the electric field from a back-gate electrode. The probe tip¨Cinduced deformation created a localized strain field in the graphene lattice. STS measurements on the deformed suspended graphene display an electronic spectrum completely different from that of graphene supported by a substrate. The spectrum indicates the formation of a spatially confined quantum dot, in agreement with recent predictions of confinement by strain-induced pseudomagnetic fields. 2¡¢Dislocation-Driven Deformations in Graphene £»Science 337, 209 (2012); The movement of dislocations in a crystal is the key mechanism for plastic deformation in all materials. Studies of dislocations have focused on three-dimensional materials, and there is little experimental evidence regarding the dynamics of dislocations and their impact at the atomic level on the lattice structure of graphene. We studied the dynamics of dislocation pairs in graphene, recorded with single-atom sensitivity. We examined stepwise dislocation movement along the zig-zag lattice direction mediated either by a single bond rotation or through the loss of two carbon atoms. The strain fields were determined, showing how dislocations deform graphene by elongation and compression of C-C bonds, shear, and lattice rotations. 3¡¢Field-Effect Tunneling Transistor Based on Vertical Graphene Heterostructures£»Science 335, 947 (2012); An obstacle to the use of graphene as an alternative to silicon electronics has been the absence of an energy gap between its conduction and valence bands, which makes it difficult to achieve low power dissipation in the OFF state. We report a bipolar field-effect transistor that exploits the low density of states in graphene and its one-atomic-layer thickness. Our prototype devices are graphene terostructures with atomically thin boron nitride or molybdenum disulfide acting as a vertical transport barrier. They exhibit room-temperature switching ratios of ¡Ö50 and ¡Ö10,000, respectively. Such devices have potential for high-frequency operation and large-scale integration.[ Last edited by º£ÌìÌìÒâ on 2012-7-26 at 23:30 ] |
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- ¸½¼þ 2 : Dislocation-DrivenDeformationsinGraphene.pdf
- ¸½¼þ 3 : Field-EffectTunnelingTransistorBasedonVerticalGraphene.pdf
2012-07-26 14:58:59, 1.05 M
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