electronic properties of graphene pdf

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electronic properties of graphene pdf

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/Name/F13 45 0 obj x���r�F�]U��-� 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 644 840 787 711 682 763 735 787 735 787 endobj 633 687 714 756 339] 1014 778 278 500] 446 453 446 631 600 815 600 600 508 569 1139 569 569 569 0 0 0 0 0 0 0 0 0 0 0 0 525 525] << /Type/Font /Type/Font endobj /BaseFont/HRIOHW+CMSY10 596 626 651 278] /FirstChar 33 935 611 1078 1207 935 352 611] /Type/Font /FontDescriptor 14 0 R /Subtype/Type1 << 2. xڽZKs�F���-`��` �(� ��e�����= (0���B����{�=\~�V�����ͷ��J)?3fus��?Qf��Y�n. /LastChar 196 /Widths[525 525 525 525 525 525 525 525 525 525 525 525 525 525 525 525 525 525 525 /Name/F14 In conclusion, some electronic properties of graphene are introduced. The interest in graphene is not only limited to the scientific community. << >> endobj /BaseFont/GKAMUC+CMR9 /FirstChar 33 /Name/F10 563 563 563 563 563 563 313 313 343 875 531 531 875 850 800 813 862 738 707 884 880 /LastChar 196 << 9 0 obj /Type/Font 295 531 295 295 531 590 472 590 472 325 531 590 295 325 561 295 885 590 531 590 561 h�bbd``b`n�@�� H�L��q��r-+H�1012��30C�g�` a� All these interesting properties make graphene a key material in condensed matter physics. %PDF-1.4 A hallmark of graphene is its unconventional electronic spectrum (Fig. 525 525 525 525 525 525 525 525 525 525 525 525 525 525 525 525 525 525 525 525 525 This leads to remarkable electronic properties of this material that have been revealed by transport measurements [1,4,5]. /FontDescriptor 8 0 R /FirstChar 33 �E��(|��k����C��/vϏV)f�v�2�����b^qY�F{yۃ�~��Bmэ���u�ԕێ:���;�^t}KK��9. "�L��L�*�5��I�"+���)`]f�xZT�i��noub��t3�Jjs+sQ�P�p���TE&��?U�п��+܈��u��}�!�"U�_-�$���Y�D3�(�ʊ*eQ. /Subtype/Type1 /BaseFont/PJCVBJ+CMMI10 896 443 624 929 754 1091 896 935 819 935 883 676 870 896 896 1220 896 896 741 352 778 778 0 0 778 778 778 1000 500 500 778 778 778 778 778 778 778 778 778 778 778 0 0 813 656 625 625 938 938 313 344 563 563 563 563 563 850 500 574 813 875 563 1019 /Widths[360 618 986 592 986 920 329 460 460 592 920 329 394 329 592 592 592 592 592 0 0 742 600 571 571 856 856 285 314 514 514 514 514 514 771 457 514 742 799 514 928 1042 799 285 514] 500 500 500 500 500 500 500 278 278 778 500 778 500 531 750 759 715 828 738 643 786 The discussion of graphene’s electronic properties and how such relativistic effects are revealed in electric transport measurements is naturally a prominent part of the present lecture notes. 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 711 986 920 827 789 924 855 920 855 920 15 0 obj 18 0 obj 361 514 778 625 917 750 778 681 778 736 556 722 750 750 1028 750 750 611 278 500 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 642 856 799 714 685 771 742 799 742 799 << /Subtype/Type1 611 611 611 611 611 611 611 352 352 352 935 579 579 935 896 851 870 916 819 786 942 0 0 722 583 556 556 833 833 278 306 500 500 500 500 500 750 444 500 722 778 500 903 400 1028 1028 424 544 440 445 533 478 499 490 592 352 420 535 307 905 620 498 516 The presence of edges in graphene has strong implications for the low-energy spectrum of the π-electrons [7]–[9]. 1 0 obj 589 524 530 539 432 675 571 826 648 579 546 399 442 730 585 339 0 0 0 0 0 0 0 0 0 /FirstChar 33 315 525 315 315 525 472 472 525 472 315 472 525 315 315 472 262 840 577 525 525 472 /FontDescriptor 23 0 R Electronics Properties Graphene is a semi-metal or zero-gap semiconductor. /Name/F8 >> 612 641 671 285] /FirstChar 33 725 667 667 667 667 667 611 611 444 444 444 444 500 500 389 389 278 500 500 611 500 /Type/Font << /Subtype/Type1 << 446 611 926 711 1122 924 889 808 889 887 657 823 909 893 1222 893 893 723 329 618 << 514 514 514 514 514 514 514 285 285 799 514 799 514 544 771 778 734 848 756 656 805 <>/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>> endobj 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. /Name/F5 531 531 531 531 531 531 295 295 295 826 502 502 826 796 752 767 811 723 693 834 796 514 514 514 514 514 514 285 285 285 799 485 485 799 771 728 742 785 699 671 806 771 446 451 469 361 572 485 716 572 490 465 322 384 636 500 278 0 0 0 0 0 0 0 0 0 0 0 /FontDescriptor 17 0 R /LastChar 196 /FirstChar 33 459 444 438 625 594 813 594 594 500 563 1125 563 563 563 0 0 0 0 0 0 0 0 0 0 0 0 Graphene, as the first emerging 2D material, has attracted considerable attention because of its remarkable physical properties and potential applications in future electronic devices. 525 525 525 525 525 525 315 315 315 787 525 525 787 763 723 735 775 696 670 794 763 endobj /BaseFont/ZUFAJK+CMR7 endobj <> 719 595 845 545 678 762 690 1201 820 796 696 817 848 606 545 626 613 988 713 668 /Type/Font stream /Subtype/Type1 0 0 767 620 590 590 885 885 295 325 531 531 531 531 531 796 472 531 767 826 531 959

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