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7k�M�f�R�}��L���m��D�s/� 295 531 295 295 531 590 472 590 472 325 531 590 295 325 561 295 885 590 531 590 561 endobj 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 676 938 875 787 750 880 813 875 813 875 Molecular modeling with different levels and theories is now effectively used to investigate the physical, chemical, and electronic properties of … The successive miniaturization of graphene electronic devices inevitably demands clarification of the edge effects on the electronic structures and electronic transport properties of nanometer-sized graphene. /Type/Font 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 525 525 525 525 525 525 525 525 525 525 0 0 525 /Subtype/Type1 208 0 obj
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611 352 611 352 352 611 676 546 676 546 384 611 676 352 384 644 352 1000 676 611 >> Finally, we conclude with a summary in section IV. 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 625 833 778 694 667 750 722 778 722 778 Structural properties of graphene Graphene due to the in-plane sp2 hybridized orbitals has a planar honeycomb structure with 778 778 0 0 778 778 778 1000 500 500 778 778 778 778 778 778 778 778 778 778 778 endobj 500 500 500 500 500 500 278 278 278 778 472 472 778 750 708 722 764 681 653 785 750
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413 583 874 706 1028 843 877 768 877 829 631 815 843 843 1151 843 843 692 323 569 /FirstChar 33 /Name/F14 0 0 813 656 625 625 938 938 313 344 563 563 563 563 563 850 500 574 813 875 563 1019 /FontDescriptor 26 0 R /Widths[285 514 856 514 856 799 285 400 400 514 799 285 343 285 514 514 514 514 514 The Dirac electrons can be controlled by application of external electric and magnetic fields, or by altering sample geometry and/or topology. KEYWORDS Graphene, self-assembled monolayers, graphene edge functionalization, doping of graphene, transport in graphene S <>/ExtGState<>/XObject<>/ProcSet[/PDF/Text/ImageB/ImageC/ImageI] >>/Annots[ 8 0 R] /MediaBox[ 0 0 595.44 841.92] /Contents 4 0 R/Group<>/Tabs/S>>
1077 826 295 531] 525 525 525 525 525 525 525 525 525 525 525 525 525 525 525 525 525 525 525 525 525 Electronics Properties Graphene is a semi-metal or zero-gap semiconductor. /LastChar 196 electronic properties of the system, then we study the electronic behavior of the system subjected to the electric field. /LastChar 196 Electronic properties of bilayer and multilayer graphene Johan Nilsson,1,2 A. H. Castro Neto,1 F. Guinea,3 and N. M. R. Peres4 1Department of Physics, Boston University, 590 Commonwealth Avenue, Boston, Massachusetts 02215, USA 2Instituut-Lorentz, Universiteit Leiden, P.O. /Type/Font /FontDescriptor 23 0 R /FontDescriptor 47 0 R <>
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